Optical apparatus which uses a virtually imaged phased array to produce chromatic dispersion

ABSTRACT

An optical apparatus for producing chromatic dispersion. The apparatus includes a virtually imaged phased array (VIPA) generator, a mirror and a lens. The VIPA generator receives an input light at a respective wavelength and produces a corresponding collimated output light traveling from the VIPA generator in a direction determined by the wavelength of the input light, the output light thereby being spatially distinguishable from an output light produced for an input light at a different wavelength. The mirror has a cone shape, or a modified cone shape. The lens focuses the output light traveling from the VIPA generator onto the mirror so that the mirror reflects the output light. The reflected light is directed by the lens back to the VIPA generator. In this manner, the apparatus provides chromatic dispersion to the input light. The modified cone shape of the mirror can be designed so that the apparatus provides a uniform chromatic dispersion to light in the same channel of a wavelength division multiplexed light. The mirror can be moved in a direction perpendicular to an angular dispersion direction of the VIPA generator, to change the amount of chromatic dispersion provided to the input light.

CROSS-REFERENCE TO RELATED APPLICATIONS

[0001] This application is a related to U.S. application Ser. No.08/796,842, filed Feb. 7, 1997; U.S. application Ser. No. 08/685,362,filed Jul. 24, 1996; and U.S. application Ser. No. 08/910,251, filedAug. 13, 1997; and which are incorporated herein by reference.

BACKGROUND OF THE INVENTION

[0002] 1. Field of the Invention

[0003] The present invention relates to an apparatus producing chromaticdispersion, and which can be used to compensate for chromatic dispersionaccumulated in an optical fiber transmission line. More specifically,the present invention relate to an apparatus which uses a virtuallyimaged phased array to produce chromatic dispersion.

[0004] 2. Description of the Related Art

[0005]FIG. 1(A) is a diagram illustrating a conventional fiber opticcommunication system, for transmitting information via light. Referringnow to FIG. 1(A), a transmitter 30 transmits pulses 32 through anoptical fiber 34 to a receiver 36. Unfortunately, chromatic dispersion,also referred to as “wavelength dispersion”, of optical fiber 34degrades the signal quality of the system.

[0006] More specifically, as a result of chromatic dispersion, thepropagating speed of a signal in an optical fiber depends on thewavelength of the signal. For example, when a pulse with a longerwavelength (for example, a pulse with wavelengths representing a “red”color pulse) travels faster than a pulse with a shorter wavelength (forexample, a pulse with wavelengths representing a “blue” color pulse),the dispersion is typically referred to as “normal” dispersion. Bycontrast, when a pulse with a shorter wavelength (such as a blue colorpulse) is faster than a pulse with a longer wavelength (such as a redcolor pulse), the dispersion is typically referred to as “anomalous”dispersion.

[0007] Therefore, if pulse 32 consists of red and blue color pulses whenemitted from transmitter 30, pulse 32 will be split as it travelsthrough optical fiber 34 so that a separate red color pulse 38 and ablue color pulse 40 are received by receiver 36 at different times. FIG.1(A) illustrates a case of “normal” dispersion, where a red color pulsetravels faster than a blue color pulse.

[0008] As another example of pulse transmission, FIG. 1(B) is a diagramillustrating a pulse 42 having wavelength components continuously fromblue to red, and transmitted by transmitter 30. FIG. 1(C) is a diagramillustrating pulse 42 when arrived at receiver 36. Since the redcomponent and the blue component travel at different speeds, pulse 42 isbroadened in optical fiber 34 and, as illustrated by FIG. 1(C), isdistorted by chromatic dispersion. Such chromatic dispersion is verycommon in fiber optic communication systems, since all pulses include afinite range of wavelengths.

[0009] Therefore, for a fiber optic communication system to provide ahigh transmission capacity, the fiber optic communication system mustcompensate for chromatic dispersion.

[0010]FIG. 2 is a diagram illustrating a fiber optic communicationsystem having an opposite dispersion component to compensate forchromatic dispersion. Referring now to FIG. 2, generally, an oppositedispersion component 44 adds an “opposite” dispersion to a pulse tocancel dispersion caused by traveling through optical fiber 34.

[0011] There are conventional devices which can be used as oppositedispersion component 44. For example, FIG. 3 is a diagram illustrating afiber optic communication system having a dispersion compensation fiberwhich has a special cross-section index profile and thereby acts as anopposite dispersion component, to compensate for chromatic dispersion.Referring now to FIG. 3, a dispersion compensation fiber 46 provides anopposite dispersion to cancel dispersion caused by optical fiber 34.However, a dispersion compensation fiber is expensive to manufacture,and must be relatively long to sufficiently compensate for chromaticdispersion. For example, if optical fiber 34 is 100 km in length, thendispersion compensation fiber 46 should be approximately 20 to 30 km inlength.

[0012]FIG. 4 is a diagram illustrating a chirped grating for use as anopposite dispersion component, to compensate for chromatic dispersion.Referring now to FIG. 4, light traveling through an optical fiber andexperiencing chromatic dispersion is provided to an input port 48 of anoptical circulator 50 provides the light to chirped grating 52. Chirpedgrating 52 reflects the light back towards circulator 50, with differentwavelength components reflected at different distances along chirpedgrating 52 so that different wavelength components travel differentdistances to thereby compensate for chromatic dispersion. For example,chirped grating 52 can be designed so that longer wavelength componentsare reflected at a farther distance along chirped grating 52, andthereby travel a farther distance than shorter wavelength components.Circulator 50 then provides the light reflected from chirped grating 52to an output port 54. Therefore, chirped grating 52 can add oppositedispersion to a pulse.

[0013] Unfortunately, a chirped grating has a very narrow bandwidth forreflecting pulses, and therefore cannot provide a wavelength bandsufficient to compensate for light including many wavelengths, such as awavelength division multiplexed light. A number of chirped gratings maybe cascaded for wavelength multiplexed signals, but this results in anexpensive system. Instead, a chirped grating with a circulator, as inFIG. 4, is more suitable for use when a single channel is transmittedthrough a fiber optic communication system.

[0014]FIG. 5 is a diagram illustrating a conventional diffractiongrating, which can be used in producing chromatic dispersion. Referringnow to FIG. 5, a diffraction grating 56 has a grating surface 58.Parallel lights 60 having different wavelengths are incident on gratingsurface 58. Lights are reflected at each step of grating surface 58 andinterfere with each other. As a result, lights 62, 64 and 66 havingdifferent wavelengths are output from diffraction grating 56 atdifferent angles. A diffraction grating can be used in a spatial gratingpair arrangement, as discussed in more detail below, to compensate forchromatic dispersion.

[0015] More specifically, FIG. 6(A) is a diagram illustrating a spatialgrating pair arrangement for use as an opposite dispersion component, tocompensate for chromatic dispersion. Referring now to FIG. 6(A), light67 is diffracted from a first diffraction grating 68 into a light 69 forshorter wavelength and a light 70 for longer wavelength. These lights 69and 70 are then diffracted by a second diffraction grating 71 intolights propagating in the same direction. As can be seen from FIG. 6(A),wavelength components having different wavelengths travel differentdistances, to add opposite dispersion and thereby compensate forchromatic dispersion. Since longer wavelengths (such as lights 70)travel longer distance than shorter wavelengths (such as lights 69), aspatial grating pair arrangement as illustrated in FIG. 6(A) hasanomalous dispersion.

[0016]FIG. 6(B) is a diagram illustrating an additional spatial gratingpair arrangement for use as an opposite dispersion component, tocompensate for chromatic dispersion. As illustrated in FIG. 6(B), lenses72 and 74 are positioned between first and second diffraction gratings68 and 71 so that they share one of the focal points. Since longerwavelengths (such as lights 70) travel shorter distance than shorterwavelengths (such as lights 69), a spatial grating pair arrangement asillustrated in FIG. 6(B) has normal dispersion.

[0017] A spatial grating pair arrangement as illustrated in FIGS. 6(A)and 6(B) is typically used to control dispersion in a laser resonator.However, a practical spatial grating pair arrangement cannot provide alarge enough dispersion to compensate for the relatively large amount ofchromatic dispersion occurring in a fiber optic communication system.More specifically, the angular dispersion produced by a diffractiongrating is usually extremely small, and is typically approximately 0.05degrees/nm. Therefore, to compensate for chromatic dispersion occurringin a fiber optic communication system, first and second gratings 68 and71 would have to be separated by very large distances, thereby makingsuch a spatial grating pair arrangement impractical.

SUMMARY OF THE INVENTION

[0018] Therefore, it is an object of the present invention to provide anapparatus which produces chromatic dispersion, and which is practicalfor compensating for chromatic dispersion accumulated in an opticalfiber.

[0019] Objects of the present invention are achieved by providing anapparatus which includes a device herein referred to as a “virtuallyimaged phased array”, “VIPA” or “VIPA generator”. The VIPA generatorproduces a light propagating away from the VIPA generator. The apparatusalso includes a mirror or reflecting surface which returns the lightback to the VIPA generator to undergo multiple reflection inside theVIPA generator.

[0020] Objects of the present invention are achieved by providing anapparatus comprising a VIPA generator and a reflecting surface. The VIPAgenerator receives an input light at a respective wavelength andproduces a corresponding collimated output light traveling from the VIPAgenerator in a direction determined by the wavelength of the inputlight. The reflecting surface reflects the output light back to the VIPAgenerator. The reflecting surface has different curvatures at differentpositions along a direction perpendicular to an angular dispersiondirection of the VIPA generator, or a plane which includes the travelingdirections of collimated output light from the VIPA generator for inputlight at different wavelengths.

[0021] Objects of the present invention are also achieved by providingan apparatus which includes a VIPA generator, a reflecting surface, anda lens. The VIPA generator receives an input light at a respectivewavelength and produces a corresponding collimated output lighttraveling from the VIPA generator in a direction determined by thewavelength of the input light, the output light thereby being spatiallydistinguishable from an output light produced for an input light at adifferent wavelength. The reflecting surface has a cone shape, or amodified cone shape. The lens focuses the output light traveling fromthe VIPA generator onto the reflecting surface so that the reflectingsurface reflects the output light, the reflected light being directed bythe lens back to the VIPA generator. The modified cone shape can bedesigned so tat the apparatus provides a uniform chromatic dispersion tolight in the same channel of a wavelength division multiplexed light.

[0022] Objects of the present invention are achieved by providing anapparatus comprising an angular dispersive component and a reflectingsurface. The angular dispersive component has a passage area to receivelight into, and to output light from, the angular dispersive component.The angular dispersive component receives, through the passage area, aninput light having a respective wavelength within a continuous range ofwavelengths, and causes multiple reflection of the input light toproduce self-interference that forms a collimated output light whichtravels from the angular dispersive component along a directiondetermined by the wavelength of the input light and is thereby spatiallydistinguishable from an output light formed for an input light havingany other wavelength within the continuous range of wavelengths. Thereflecting surface reflects the output light back to the angulardispersive component to undergo multiple reflection in the angulardispersive component and then be output from the passage area. Thereflecting surface has different curvatures at different positions alonga direction which is perpendicular to a plane which includes the traveldirection of collimated output light from the angular dispersivecomponent for input light at different wavelengths.

[0023] Moreover, objects of the present invention are achieved byproviding an apparatus which includes an angular dispersive componentand a reflecting surface. The angular dispersive component has a passagearea to receive light into, and to output light from, the angulardispersive component. The angular dispersive component receives, throughthe passage area, a line focused input light and causes multiplereflection of the input light to produce self-interference that forms acollimated output light which travels from the angular dispersivecomponent along a direction determined by the wavelength of the inputlight and is thereby spatially distinguishable from an output lightformed for an input light having a different wavelength. The reflectingsurface reflects the output light back to the angular dispersivecomponent to undergo multiple reflection in the angular dispersivecomponent and then be output from the passage area. The reflectingsurface has different curvatures at different positions along adirection which is perpendicular to a plane which includes the traveldirection of collimated output light from the angular dispersivecomponent for input light at different wavelengths.

[0024] Objects of the present invention are still further achieved byproviding an apparatus comprising first and second reflecting surfaces,and a mirror. The second reflecting surface has a reflectivity whichcauses a portion of light incident thereon to be transmittedtherethrough. An input light at a respective wavelength is focused intoa line. The first and second reflecting surfaces are positioned so thatthe input light radiates from the line to be reflected a plurality oftimes between the first and second reflecting surfaces and thereby causea plurality of lights to be transmitted through the second reflectingsurface. The plurality of transmitted lights interfere with each otherto produce a collimated output light which travels from the secondreflecting surface along a direction determined by the wavelength of theinput light, and is thereby specially distinguishable from an outputlight formed for an input light having a different wavelength. Themirror surface reflects output the light back to the second reflectingsurface to pass through the second reflecting surface and undergomultiple reflection between the first and second reflecting surfaces.The mirror surface has different curvatures at different positions alonga direction which is perpendicular to a plane which includes the traveldirection of collimated output light from the second reflecting surfacefor input light at different wavelengths.

[0025] Objects of the present invention are also achieved by providingan apparatus which includes a VIPA generator, a lens, first and secondmirrors, and a wavelength filter. The VIPA generator receives a linefocused wavelength division multiplexed (WDM) light including light atfirst and second wavelengths, and produces collimated first and secondoutput lights corresponding, respectively, to the first and secondwavelengths. The first and second output lights travel from the VIPAgenerator in first and second directions, respectively, determined bythe first and second wavelengths, respectively. The lens focuses thefirst and second output lights traveling from the VIPA generator. Thefirst and second mirrors each having a cone shape or a modified coneshape for producing a uniform chromatic dispersion. The wavelengthfilter filters light focused by the lens so that light at the firstwavelength is focused to the first mirror and reflected by the firstmirror, and light at the second wavelength is focused to the secondmirror and reflected by the second mirror. The reflected first andsecond lights are directed by the wavelength filter and the lens back tothe VIPA generator.

[0026] Moreover, objects of the present invention are achieved bycausing the input light to have a double-hump shaped far fielddistribution. For example, a phase mask can be provided on an inputfiber, or on a surface of the VIPA generator, to cause the input lightto have a double-hump shaped far field distribution.

BRIEF DESCRIPTION OF THE DRAWINGS

[0027] These and other objects and advantages of the invention willbecome apparent and more readily appreciated from the followingdescription of the preferred embodiments, taken in conjunction with theaccompanying drawings of which:

[0028]FIG. 1(A) (prior art) is a diagram illustrating a conventionalfiber optic communication system.

[0029]FIG. 1(B) is a diagram illustrating a pulse before transmissionthrough a fiber in a conventional fiber optic communication system.

[0030]FIG. 1(C) is a diagram illustrating a pulse after beingtransmitted through a fiber in a conventional fiber optic communicationsystem.

[0031]FIG. 2 (prior art) is a diagram illustrating a fiber opticcommunication system having an opposite dispersion component tocompensate for chromatic dispersion.

[0032]FIG. 3 (prior art) is a diagram illustrating a fiber opticcommunication system having a dispersion compensation fiber as anopposite dispersion component.

[0033]FIG. 4 (prior art) is a diagram illustrating a chirped grating foruse as an opposite dispersion component, to compensate for chromaticdispersion.

[0034]FIG. 5 (prior art) is a diagram illustrating a conventionaldiffraction grating.

[0035]FIG. 6(A) (prior art) is a diagram illustrating a spatial gratingpair arrangement for production of anomalous dispersion.

[0036]FIG. 6(B) (prior art) is a diagram illustrating a spatial gratingpair arrangement for production of normal dispersion.

[0037]FIG. 7 is a diagram illustrating a VIPA.

[0038]FIG. 8 is a detailed diagram illustrating the VIPA of FIG. 7.

[0039]FIG. 9 is a diagram illustrating a cross-section along lines IX-IXof the VIPA illustrated in FIG. 7.

[0040]FIG. 10 is a diagram illustrating interference between reflectionsproduced by a VIPA.

[0041]FIG. 11 is a diagram illustrating a cross-section along linesIX-IX of the VIPA illustrated in FIG. 7, for determining the tilt angleof input light.

[0042] FIGS. 12(A), 12(B), 12(C) and 12(D) are diagrams illustrating amethod for producing a VIPA.

[0043]FIG. 13 is a diagram illustrating an apparatus which uses a VIPAas an angular dispersion component to produce chromatic dispersion.

[0044]FIG. 14 is a more detailed diagram illustrating the operation ofthe apparatus in FIG. 13.

[0045]FIG. 15 is a diagram illustrating various orders of interferenceof a VIPA.

[0046]FIG. 16 is a graph illustrating the chromatic dispersion forseveral channels of a wavelength division multiplexed light.

[0047]FIG. 17 is a diagram illustrating different channels of awavelength division multiplexed light being focused at different pointson a mirror by a VIPA.

[0048]FIG. 18 is a diagram illustrating aside view of an apparatus whichuses a VIPA to provide variable chromatic dispersion to light.

[0049]FIG. 19 is a diagram illustrating a side view of an apparatuswhich uses a VIPA to provide variable chromatic dispersion to light.

[0050] FIGS. 20(A) and 20(B) are diagrams illustrating side views of anapparatus which uses a VIPA to provide chromatic dispersion to light.

[0051]FIG. 21 is a graph illustrating the output angle of a luminousflux from a VIPA versus wavelength of the luminous flux.

[0052]FIG. 22 is a graph illustrating the angular dispersion of a VIPAversus the wavelength of a luminous flux.

[0053]FIG. 23 is a graph illustrating the effect of different mirrortypes in an apparatus using a VIPA.

[0054]FIG. 24 is a diagram illustrating chromatic dispersion versuswavelength in an apparatus using a VIPA, for different types of mirrorsused in the apparatus.

[0055]FIG. 25 is a graph illustrating the effect of a mirror in anapparatus which uses a VIPA.

[0056] PIG. 26 is a graph illustrating constant chromatic dispersion ofan apparatus using a VIPA.

[0057]FIG. 27 is a graph illustrating characteristics of differentmirror designs for an apparatus using a VIPA.

[0058] FIGS. 28(A), 28(B), 28(C), 28(D), 28(E) and 28(F) are diagramsillustrating examples of mirrors of an apparatus using a VIPA.

[0059]FIG. 29 is a diagram illustrating a cylindrical mirror.

[0060]FIG. 30(A) is a graph illustrating chromatic dispersion versuswavelength for one channel of a wavelength division multiplexed light,after undergoing chromatic dispersion compensation with a VIPA with acylindrical mirror.

[0061]FIG. 30(B) is a graph illustrating chromatic dispersion versuswavelength for all wavelengths of a wavelength division multiplexedlight, after undergoing chromatic dispersion compensation with a VIPAwith a cylindrical mirror.

[0062]FIG. 31(A) is a graph illustrating chromatic dispersion versuswavelength for one channel of a wavelength division multiplexed light,after undergoing chromatic dispersion compensation with a VIPA with amodified cylindrical mirror.

[0063]FIG. 31(B) is a graph illustrating chromatic dispersion versuswavelength for all wavelengths of a wavelength division multiplexedlight, after undergoing chromatic dispersion compensation with a VIPAwith a modified cylindrical mirror.

[0064]FIG. 32 is a diagram illustrating a top view of an apparatus usinga VIPA to provide variable chromatic dispersion to light, according to afurther embodiment of the present invention.

[0065] FIGS. 33(A) and 33(B) are diagrams illustrating how a mirror canbe formed from a section of a cone, according to an embodiment of thepresent invention.

[0066]FIG. 34(A) is a graph illustrating the amount of chromaticdispersion versus wavelength within one channel for different radii ofcurvature of a mirror in an apparatus using a VIPA to provide chromaticdispersion, according to an embodiment of the present invention.

[0067]FIG. 34(B) is a diagram illustrating radii of curvature of FIG.34(A), according to an embodiment of the present invention.

[0068]FIG. 34(C) is a diagram illustrating modified radii of curvature,according to an embodiment of the present invention.

[0069]FIG. 35 is a graph illustrating the chromatic dispersion versuswavelength for different radii of curvature in an apparatus using a VIPAto provide chromatic dispersion, according to an embodiment of thepresent invention.

[0070]FIG. 36 is a diagram illustrating various angles in an apparatuswhich uses a VIPA, according to an embodiment of the present invention.

[0071]FIG. 37 is an additional diagram illustrating angles in anapparatus which uses a VIPA, according to an embodiment of the presentinvention.

[0072]FIG. 38 is a diagram illustrating how chromatic dispersion isgenerated in an apparatus using a VIPA, according to an embodiment ofthe present invention.

[0073] FIGS. 39(A), 39(B) and 39(C) are graphs illustrating mirrorcurves, according to an embodiment of the present invention.

[0074]FIG. 40 is a diagram illustrating a cone for forming a mirror,according to an embodiment of the present invention.

[0075]FIG. 41 is a diagram illustrating a step shaped mirror surface,according to an embodiment of the present invention.

[0076]FIG. 42 is a diagram illustrating a side view of an apparatususing a VIPA to provide chromatic dispersion slope, according to anadditional embodiment of the present invention.

[0077]FIG. 43(A) is a graph illustrating the amount of chromaticdispersion for all wavelengths with the apparatus in FIG. 42 using acone shaped mirror, according to an embodiment of the present invention.

[0078]FIG. 43(B) is a graph illustrating the amount of chromaticdispersion for all wavelengths with the apparatus in FIG. 42 using amodified cone shaped mirror, according to an embodiment of the presentinvention.

[0079]FIG. 44 is a diagram illustrating the use of a holographic gratingbetween a VIPA and a lens, according to an embodiment of the presentinvention.

[0080]FIG. 45 is a diagram illustrating the use of a reflection typegrating between a VIPA and a lens, according to an embodiment of thepresent invention.

[0081]FIGS. 46 and 47 are diagrams illustrating the use of quarter waveplate, according to embodiments of the present invention.

[0082]FIG. 48(A) is a diagram illustrating a side or top view of anapparatus which uses a VIPA to provide different chromatic dispersionfor different channels, according to a still further embodiment of thepresent invention.

[0083]FIG. 48(B) is a graph illustrating chromatic dispersion versuswavelength for the apparatus in FIG. 48(A), according to an embodimentof the present invention.

[0084]FIG. 49 is a diagram illustrating a side or top view of anapparatus which uses a VIPA to provide different chromatic dispersionfor different channels, according to an embodiment of the presentinvention.

[0085]FIG. 50 is a graph illustrating insertion loss in an apparatuswhich uses a VIPA to provide chromatic dispersion, according to anembodiment of the present invention.

[0086]FIG. 51 is a diagram illustrating different diffraction efficiencyat different wavelengths in an apparatus which uses a VIPA to providechromatic dispersion, according to an embodiment of the presentinvention.

[0087]FIG. 52 is a diagram illustrating the light intensity of lighttraveling out of a fiber and into a VIPA, according to an embodiment ofthe present invention.

[0088]FIG. 53 is ad illustrating a side view of an optical phase mask onan input fiber to produce a double-humped shape far field distribution,in an apparatus which uses a VIPA to provide chromatic dispersion,according to an embodiment of the present invention.

[0089]FIG. 54 is a diagram illustrating a cross-sectional view alonglines 54-54 in FIG. 53, according to an embodiment of the presentinvention.

[0090]FIG. 55 is a diagram illustrating a side view of phase masks on aVIPA to provide a double-humped shape far field distribution withrespect to light received inside the VIPA, according to an embodiment ofthe present invention.

[0091]FIG. 56 is a diagram illustrating a side view of phase masks on aVIPA to provide a double-humped shape far field distribution withrespect to light received inside the VIPA, according to an additionalembodiment of the present invention.

[0092]FIGS. 57 and 58 are diagrams illustrating a side view of phasemasks on a VIPA to provide a double-humped shape far field distributionwith respect to light received inside the VIPA, according to anadditional embodiment of the present invention.

[0093]FIG. 59 is a diagram illustrating excessive loss added to a losscurve, according to an embodiment of the present invention.

[0094]FIG. 60 is a diagram illustrating the use of an excess losscomponent to provide excess loss, according to an embodiment of thepresent invention.

[0095]FIG. 61 is a diagram illustrating a side view of a mirror for usewith a VIPA to provide chromatic dispersion, according to an embodimentof the present invention.

[0096]FIG. 62 is a diagram illustrating a front view of a mirror,according to an embodiment of the present invention.

[0097] FIGS. 63(A), 63(B) and 63(C) are diagrams illustrating a way tomodulate effective reflectivity in an apparatus using a VIPA, accordingto an embodiment of the present invention.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

[0098] Reference will now be made in detail to the present preferredembodiments of the present invention, examples of which are illustratedin the accompanying drawings, wherein like reference numerals refer tolike elements throughout.

[0099]FIG. 7 is a diagram illustrating a virtually imaged phased array(VIPA). Moreover, hereinafter, the terms “virtually imaged phasedarray,” “VIPA” and “VIPA generator” may be used interchangeably.

[0100] Referring now to FIG. 7, a VIPA 76 is preferably made of a thinplate of glass. An input light 77 is focused into a line 78 with a lens80, such as a semi-cylindrical lens, so that input light 77 travels intoVIPA 76. Line 78 is hereinafter referred to as “focal line 78”. Inputlight 77 radially propagates from focal line 78 to be received insideVIPA 76. VIPA 78 then outputs a luminous flux 82 of collimated light,where the output angle of luminous flux 82 varies as the wavelength ofinput light 77 changes. For example, when input light 77 is at awavelength λ1, VIPA 76 outputs a luminous flux 82 a at wavelength λ1 ina specific direction. When input light 77 is at a wavelength λ2, VIPA 76outputs a luminous flux 82 b at wavelength λ2 in a different direction.Therefore, VIPA 76 produces luminous fluxes 81 a and 81 b which arespatially distinguishable from each other.

[0101]FIG. 8 is a detailed diagram illustrating VIPA 76. Referring nowto FIG. 8, VIPA 76 includes a plate 120 made of, for example, glass, andhaving reflecting films 122 and 124 thereon. Reflecting film 122preferably has a reflectance of approximately 95% or higher, but lessthan 100%. Reflecting film 124 preferably has a reflectance ofapproximately 100%. A radiation window 126 is formed on plate 120 andpreferably has a reflectance of approximately 0% reflectance.

[0102] Input light 77 is focused into focal line 78 by lens 80 throughradiation window 126, to undergo multiple reflection between reflectingfilms 122 and 124. Focal line 78 is preferably on the surface of plate120 to which reflecting film 122 is applied. Thus, focal line 78 isessentially line focused onto reflecting film 122 through radiationwindow 126. The width of focal line 78 can be referred to as the “beamwaist” of input light 77 as focused by lens 80. Thus, the embodiment ofthe present invention as illustrated is FIG. 8 focuses the beam waist ofinput light 77 onto the far surface (that is, the surface havingreflecting film 122 thereon) of plate 120. By focusing the beam waist onthe far surface of plate 120, the present embodiment of the presentinvention reduces the possibility of overlap between (i) the area ofradiation window 126 on the surface of plate 120 covered by input light77 as it travels through radiation window 126 (for example, the area “a”illustrated in FIG. 11, discussed in more detail further below), and(ii) the area on reflecting film 124 covered by input light 77 wheninput light 77 is reflected for the first time by reflecting film 124(for example, the area “b” illustrated in FIG. 11, discussed in moredetail further below). It is desirable to reduce such overlap to ensureproper operation of the VIPA.

[0103] In FIG. 8, an optical axis 132 of input light 77 has a small tiltangle θ. Upon the first reflection off of reflecting film 122, 5% of thelight passes through reflecting film 122 and diverges after the beamwaist, and 95% of the light is reflected towards reflecting film 124.After being reflecting by reflecting film 124 for the first time, thelight again hits reflecting film 122 but is displaced by an amount d.Then, 5% of the light passes through reflecting film 122. In a similarmanner, as illustrated in FIG. 8, the light is split into many pathswith a constant separation d. The beam shape hi each path forms so thatthe light diverges from virtual images 134 of the beam waist. Virtualimages 134 are located with constant spacing 2t along a line that isnormal to plate 120, where t is the thickness of plate 120. Thepositions of the beam waists in virtual images 134 are self-aligned, andthere is no need to adjust individual positions. The lights divergingfrom virtual images 134 interfere with each other and form collimatedlight 136 which propagates in a direction that changes in accordancewith the wavelength of input light 77.

[0104] The spacing of light paths is d=2t Sin θ, and the difference inthe path lengths between adjacent beams is 2t Cos θ. The angulardispersion is proportional to the ratio of these two numbers, which iscot θ. As a result, a VIPA produces a significantly large angulardispersion.

[0105] As easily seen from FIG. 8, the term “virtually imaged phasedarray” arises from the formation of an array of virtual images 134.

[0106]FIG. 9 is a diagram illustrating a cross-section along lines IX-IXof VIPA 76 illustrated in FIG. 7. Referring now to FIG. 9, plate 120 hasreflecting surfaces 122 and 124 thereon. Reflecting surfaces 122 and 124are in parallel with each other and spaced by the thickness t of plate120. Reflecting surfaces 122 and 124 are typically reflecting filmsdeposited on plate 120. As previously described, reflecting surface 124has a reflectance of approximately 100%, except in radiation window 126,and reflecting surface 122 has a reflectance of approximately 95% orhigher. Therefore, reflecting surface 122 has a transmittance ofapproximately 5% or less so that approximately 5% of less of lightincident on reflecting surface 122 will be transmitted therethrough andapproximately 95% or more of the light will be reflected. Thereflectances of reflecting surfaces 122 and 124 can easily be changed inaccordance with the specific VIPA application. However, generally,reflecting surface 122 should have a reflectance which is less than 100%so that a portion of incident light can be transmitted therethrough.

[0107] Reflecting surface 124 has radiation window 126 thereon.Radiation window 126 allows light to pass therethrough, and preferablyhas no reflectance, or a very low reflectance. Radiation window 126receives input light 77 to allow input light 77 to be received between,and reflected between, reflecting surfaces 122 and 124.

[0108] Since FIG. 9 represents a cross-section along lines IX-IX in FIG.7, focal line 78 in FIG. 7 appears as a “point” in FIG. 9. Input light77 then propagates radially from focal line 78. Moreover, as illustratedin FIG. 9, focal line 78 is positioned on reflecting surface 122.Although it is not required for focal line 78 to be on reflectingsurface 122, a shift in the positioning of focal line 78 may cause smallchanges in the characteristics of VIPA 76.

[0109] As illustrated in FIG. 9, input light 77 enters plate 120 throughan area A0 in radiation window 126, where points P0 indicate peripheralpoints of area A0.

[0110] Due to the reflectivity of reflecting surface 122, approximately95% or more of input light 77 is reflected by reflecting surface 122 andis incident on area A1 of reflecting surface 124. Points P1 indicateperipheral points of area A1. After reflecting off area A1 on reflectingsurface 124, input light 77 travels to reflecting surface 122 and ispartially transmitted trough reflecting surface 122 as output light Out1defined by rays R1. In this manner, as illustrated in FIG. 9, inputlight 77 experiences multiple reflections between reflecting surfaces122 and 124, wherein each reflection off of reflecting surface 122 alsoresults in a respective output light being transmitted therethrough.Therefore, for example, each time immediately after input light 77reflects off of areas A2, A3 and A4 on reflecting surface 124, inputlight 77 reflects off of reflecting surface 122 to produce output lightsOut2, Out3 and Out4. Points P2 indicate peripheral points of area A2,points P3 indicate peripheral points of area A3, and points P4 indicateperipheral points of area A4. Output light Out2 is defined by rays R2,output light Out3 is defined by rays R3 and output light Out4 is definedby rays R4. Although FIG. 9 only illustrates output lights Out0, Out1,Out2, Out3 and Out4, there will actually be many more output lights,depending on the power on input light 77 and the reflectances ofreflecting surfaces 122 and 124. As will be discussed in more detailfurther below, the output lights interfere with each other to produce aluminous flux having a direction which changes in accordance with thewavelength of input light 77. Therefore, the luminous flux can bedescribed as being a resulting output light formed from the interferenceof output lights Out0, Out1, Out2, Out3 and Out4.

[0111]FIG. 10 is a diagram illustrating interference between reflectionsproduced by a VIPA. Referring now to FIG. 10, light traveling from focalline 78 is reflected by reflecting surface 124. As previously described,reflecting surface 124 has a reflectance of approximately 100% and,therefore, functions essentially as a mirror. As a result, output lightOut1 can be optically analyzed as if reflecting surfaces 122 and 124 didnot exist and, instead, output light Out1 was emitted from a focal lineI₁. Similarly, output lights Out2, Out3 and Out4 can beoptically-analyzed as if they were emitted from focal lines I₁, I₂, I₃and I₄, respectively. The focal lines I₂, I₃ and I₄ are virtual imagesof a focal line I₀.

[0112] Therefore, as illustrated in FIG. 10, focal line I₁ is a distance2t from focal line I₀, where t equals the distance between reflectingsurfaces 122 and 124. Similarly, each subsequent focal line is adistance 2t from the immediately preceding focal line. Thus, focal lineI₂ is a distance 2t from focal line I₁. Moreover, each subsequentmultiple reflection between reflecting surfaces 122 and 124 produces anoutput light which is weaker in intensity than the previous outputlight. Therefore, output light Out2 is weaker in intensity than outputlight Out1.

[0113] As illustrated in FIG. 10, output lights from the focal linesoverlap and interfere with each other. More specifically, since focallines I₁, I₂, I₃ and I₄ are the virtual images of focal line I₀, outputlights Out0, Out1, Out2, Out3 and Out4 have the same optical phase atthe positions of focal lines I₁, I₂, I₃ and I₄. Therefore, interferenceproduces a luminous flux which travels in a specific direction dependingon the wavelength of input light 77.

[0114] A VIPA according to the above embodiments of the presentinvention has strengthening conditions which are characteristics of thedesign of the VIPA. The strengthening conditions increase theinterference of the output lights so that a luminous flux is formed. Thestrengthening conditions of the VIPA are represented by the followingEquation (1):

2t×cosφ=mλ

[0115] where φ indicates the propagation direction of the resultingluminous flux as measured from a line perpendicular to the surface ofreflecting surfaces 122 and 124, λ indicates the wavelength of the inputlight, t indicates the distance between the reflecting surfaces 122 and124, and m indicates an integer.

[0116] Therefore, if t is constant and m is assigned a specific value,then the propagation direction φ of the luminous flux formed for inputlight having wavelength λ can be determined.

[0117] More specifically, input light 77 is radially dispersed fromfocal line 78 through a specific angle. Therefore, input light havingthe same wavelength will be traveling in many different direction fromfocal line 78, to be reflected between reflecting surfaces 122 and 124.The strengthening conditions of the VIPA cause light traveling in aspecific direction to be strengthened through interference of the outputlights to form a luminous flux having a direction corresponding to thewavelength of the input light. Light traveling in different directionthan the specific direction required by the strengthening condition willbe weakened by the interference of the output lights.

[0118]FIG. 11 is a diagram illustrating a cross-section along linesIX-IX of the VIPA illustrated in FIG. 7, showing characteristic of aVIPA for determining the angle of incidence, or tilt angle, of inputlight.

[0119] Referring now to FIG. 11, input light 77 is collected by acylindrical lens (not illustrated) and focused at focal line 78. Asillustrated in FIG. 11, input light 77 covers an area having a widthequal to “a” on radiation window 126. After input light 77 is reflectedone time from reflecting surface 122, input light 77 is incident onreflecting surface 124 and covers an area having a width equal to “b” onreflecting surface 124. Moreover, as illustrated in FIG. 11, input light77 travels along optical axis 132 which is at a tilt angle θ1 withrespect to the normal to reflecting surface 122.

[0120] The tilt angle θ1 should be set to prevent input light 77 fromtraveling out of the plate through radiation window 126 after beingreflected the first time by reflecting surface 122. In other words, thetilt angle θ1 should be set so that input light 77 remains “trapped”between reflecting surfaces 122 and 124 and does not escape throughradiation window 126. Therefore, to prevent input light 77 fromtraveling out of the plate through radiation window 126, the tilt angleθ1 should be set in accordance with the following Equation (2):

tilt of optical axis θ1≧(a+b)/4t

[0121] Therefore, as illustrated by FIGS. 7-11, a VIPA receives an inputlight having a respective wavelength within a continuous range ofwavelengths. The VIPA causes multiple reflection of the input light toproduce self-interference and thereby form an output light. The outputlight is spatially distinguishable from an output light formed for aninput light having any other wavelength within the continuous range ofwavelengths. For example, FIG. 9 illustrates an input light 77 whichexperiences multiple reflection between reflecting surfaces 122 and 124.This multiple reflection produces a plurality of output lights Out0,Out1, Out2, Out3 and Out 4 which interfere with each other to produce aspatially distinguishable luminous flux for each wavelength of inputlight 77.

[0122] “Self-interference” is a term indicating that interference occursbetween a plurality of lights or beams which all originate from the samesource. Therefore, the interference of output lights Out0, Out1, Out2,Out3 and Out4 is referred to as self-interference of input light 77,since output lights Out0, Out1, Out2, Out3 and Out4 all originate fromthe same source (that is, input light 77).

[0123] An input light can be at any wavelength within a continuous rangeof wavelengths. Thus, the input light is not limited to being awavelength which is a value chosen from a range of discrete values. Inaddition, the output light produced for an input light at a specificwavelength within a continuous range of wavelengths is spatiallydistinguishable from an output light which would have been produced ifthe input light was at a different wavelength within the continuousrange of wavelengths. Therefore, as illustrated, for example, in FIG. 7,the traveling direction (that is, a “spatial characteristic”) of theluminous flux 82 is different when input light 77 is at differentwavelengths within a continuous range of wavelengths.

[0124] FIGS. 12(A), 12(B), 12(C) and 12(D) are diagram illustrating amethod for producing a VIPA.

[0125] Referring now to FIG. 12(A), a parallel plate 164 is preferablymade of glass and exhibits excellent parallelism. Reflecting films 166and 168 are formed on both sides of the parallel plate 164 by vacuumdeposition, ion spattering or other such methods. One of reflectingfilms 166 and 168 has a reflectance of nearly 100%, and the otherreflecting film has a reflectance of lower than 100%, and preferablyhigher than 80%.

[0126] Referring now to FIG. 12(B), one of reflecting films 166 and 168is partially shaved off to form a radiation window 170. In FIG. 12(B),reflecting film 166 is shown as being shaved off so that radiationwindow 170 can be formed on the same surface of parallel plate 164 asreflecting film 166. However, instead, reflecting film 168 can bepartially shaved off so that a radiation window is formed on the samesurface of parallel plate 164 as reflecting film 168. As illustrated bythe various embodiment of the present invention, a radiation window canbe on either side of parallel plate 164.

[0127] Shaving off a reflecting film can be performed by an etchingprocess, but a mechanical shaving process can also be used and is lessexpensive. However, if a reflecting film is mechanically shaved,parallel plate 164 should be carefully processed to minimize damage toparallel plate 164. For example, if the portion of parallel plate 164forming the radiation window is severely damaged, parallel plate 164will generate excess loss caused by scattering of received input light.

[0128] Instead of first forming a reflecting film and then shaving itoff, a radiation window can be produced by preliminarily masking aportion of parallel plate 164 corresponding to a radiation window, andthen prong this portion from being covered with reflecting film.

[0129] Referring now to FIG. 12(C), a transparent adhesive 172 isapplied onto reflecting film 166 and the portion of parallel plate 164from which reflecting film 166 has been removed. Transparent adhesive172 should generate the smallest possible optical loss since it is alsoapplied to the portion of parallel plate 164 forming a radiation window.

[0130] Referring now to FIG. 12(D), a transparent protector plate 174 isapplied onto transparent adhesive 172 to protect reflecting film 166 andparallel plate 164. Since transparent adhesive 172 is applied to fillthe concave portion generated by removing reflecting film 166,transparent protector plate 174 can be provided in parallel with the topsurface of parallel plate 164.

[0131] Similarly, to protect reflecting film 168, an adhesive (notillustrated) can be applied to the top surface of reflecting film 168and should be provided with a protector plate (not illustrated). Ifreflecting film 168 has a reflectance of about 100%, and there is noradiation window on the same surface of parallel plate 164, then anadhesive and protector plate do not necessarily have to be transparent.

[0132] Furthermore, an anti-reflection film 176 can be applied ontransparent protector plate 174. For example, transparent protectorplate 174 and radiation window 170 can be covered with anti-reflectionfilm 176.

[0133] A focal line can be on the surface of a radiation window or onthe opposite surface of a parallel plate from which input light enters.Moreover, the focal line can be in the parallel plate, or before theradiation window.

[0134] In accordance with the above, two reflecting films reflect lighttherebetween, with the reflectance of one reflecting film beingapproximately 100%. However, a similar effect can be obtained with tworeflecting films each having a reflectance of less than 100%. Forexample, both reflecting films can have a reflectance of 95%. In thiscase, each reflecting film has light traveling therethrough and causinginterference. As a result, a luminous flux traveling in the directiondepending on the wavelength is formed on both sides of the parallelplate on which the reflecting films are formed. Thus, the variousreflectances of the various embodiments of the present invention caneasily be changed in accordance with required characteristics of a VIPA.

[0135] In accordance with the above, a waveguide device is formed by aparallel plate, or by two reflecting surfaces in parallel with eachother. However, the plate or reflecting surfaces do not necessarily haveto be parallel.

[0136] In accordance with the above, a VIPA uses multiple-reflection andmaintains a constant phase difference between interfering lights. As aresult, the characteristics of the VIPA are stable, thereby reducingoptical characteristic changes causes by polarization. By contrast, theoptical characteristics of a conventional diffraction grating experienceundesirable changes in dependance on the polarization of the inputlight.

[0137] In accordance with the above, a VIPA provides luminous fluxeswhich are “spatially distinguishable” from each other. “Spatiallydistinguishable” refers to the luminous fluxes being distinguishable inspace. For example, various luminous fluxes are spatiallydistinguishable if they are collimated and travel in differentdirections, or are focused in different locations. However, theinvention is not intended to be limited to these precise examples, andthere are many other ways in which luminous fluxes can be spatiallydistinguished from each other.

[0138]FIG. 13 is a diagram illustrating an apparatus which uses a VIPAas an angular dispersive component, instead of using diffractiongratings, to produce chromatic dispersion. Referring now to FIG. 13, aVIPA 240 has a first surface 242 with a reflectivity of, for example,approximately 100%, and a second surface 244 with a reflectivity of, forexample, approximately 98%. VIPA 240 also includes a radiation window247. However, VIPA 240 is not limited to this specific configuration.Instead, VIPA 240 can have many different configurations as describedherein.

[0139] As illustrated in FIG. 13, a light is output from a fiber 246,collimated by a collimating lens 248 and line-focused into VIPA 240through radiation window 247 by a cylindrical lens 250. VIPA 240 thenproduces a collimated light 251 which is focused by a focusing lens 252onto a mirror 254. Mirror 254 can be a mirror portion 256 formed on asubstrate 258.

[0140] Mirror 254 reflects the light back through focusing lens 252 intoVIPA 240. The light then undergoes multiple reflections in VIPA 240 andis output from radiation window 247. The light output from radiationwindow 247 travels through cylindrical lens 250 and collimating lens 248and is received by fiber 246.

[0141] Therefore, light is output from VIPA 240 and reflected by mirror254 back into VIPA 240. The light reflected by mirror 254 travelsthrough the path which is exactly opposite in direction to the paththrough which it originally traveled. As will be seen in more detailbelow, different wavelength components in the light are focused ontodifferent positions on mirror 254, and are reflected back to VIPA 240.As a result, different wavelength components travel different distances,to thereby produce chromatic dispersion.

[0142]FIG. 14 is a more detailed diagram illustrating the operation ofthe VIPA in FIG. 13. Assume a light having various wavelength componentsis received by VIPA 240. As illustrated in FIG. 14, VIPA 240 will causethe formation of virtual images 260 of beam waist 262, where eachvirtual image 260 emits light.

[0143] As illustrated in FIG. 14, focusing lens 252 focuses thedifferent wavelength components in a collimated light from VIPA 240 atdifferent points on mirror 254. More specifically, a longer wavelength264 focuses at point 272, a center wavelength 266 focuses at point 270,and a shorter wavelength 268 focuses at point 274. Then, longerwavelength 264 returns to a virtual image 260 which is closer to beamwaist 262, as compared to center wavelength 266. Shorter wavelength 268returns to a virtual image 260 which is farther from beam waist 262, ascompared to center wavelength 266. Thus, the arrangement provides fornormal dispersion.

[0144] Mirror 254 is designed to reflect only light in a specificinterference order, and light in any other interference order should befocused out of mirror 254. More specifically, as previously described, aVIPA will output a collimated light. This collimate light will travel ina direction in which the path from each virtual image has a differenceof mλ, where m is an integer. The mth order of interference is definedas an output light corresponding to m.

[0145] For example, FIG. 15 is a diagram illustrating various orders ofinterference of a VIPA. Referring now to FIG. 15, a VIPA, such as VIPA240, emits collimated lights 276, 278 and 280. Each collimated light276, 278 and 280 corresponds to a different interference order.Therefore, for example, collimated light 276 is collimated lightcorresponding to an (n+2)th interference order, collimated light 278 iscollimated light corresponding to an (n+1)th interference order, andcollimated light 280 is collimated light corresponding to an nthinterference order, wherein n is an integer. Collimated light 276 isillustrated as having several wavelength components 276 a, 276 b and 276c. Similarly, collimated light 278 is illustrated as having wavelengthcomponents 278 a, 278 b and 278 c, and collimated light 280 isillustrated as having wavelength components 280 a, 280 b and 280 c.Here, wavelength components 276 a, 278 a and 280 a have the samewavelength. Wavelength components 276 b, 278 b and 280 b have the samewavelength (but different from the wavelength of wavelength components276 a, 278 a and 280 a). Wavelength components 276 c, 278 c and 280 chave the same wavelength (but different from the wavelength ofwavelength components 276 a, 278 a and 280 a, and the wavelength ofwavelength components 276 b, 278 b and 280 b). Although FIG. 15 onlyillustrates collimated light for three different interference orders,collimated lights will be emitted for many other interference orders.

[0146] Since collimated lights at the same wavelength for differentinterference orders travel in different directions and are thereforefocused at different positions, mirror 254 can be made to reflect onlylight from a single interference order back into VIPA 240. For example,as illustrated in FIG. 15, the length of a reflecting portion of mirror254 should be made relatively small, so that only light corresponding toa single interference order is reflected. More specifically, in FIG. 15,only collimated light 278 is reflected by mirror 254. In this manner,collimated lights 276 and 278 are focused out of mirror 254.

[0147] A wavelength division multiplexed light usually includes manychannels. Referring again to FIG. 13, if the thickness t between firstand second surfaces 242 and 244 of VIPA 240 is set at a specific value,the arrangement will be able to simultaneously compensate for dispersionin each channel.

[0148] More specifically, each channel has a center wavelength. Thesecenter wavelengths are usually spaced apart by a constant frequencyspacing. The thickness t of VIPA 240 between first and second surfaces242 and 244 should be set so that all of the wavelength componentscorresponding to the center wavelengths have the same output angle fromVIPA 240 and thus the same focusing position on mirror 254. This ispossible when the thickness t is set so that, for each channel, theround-trip optical length through VIPA 240 traveled by the wavelengthcomponent corresponding to the center wavelength is a multiple of thecenter wavelength of each channel. This amount of thickness t willhereafter be referred to as the “WDM matching free spectral rangethickness”, or “WDM matching FSR thickness”.

[0149] Moreover, in this case, the round-trip optical length (2nt cos θ)through VIPA 240 is equal to the wavelength corresponding to the centerwavelength in each channel multiplied by an integer for the same θ anddifferent integer, where n is the refractive index of the materialbetween first and second surfaces 242 and 244, θ indicates a propagationdirection of a luminous flux corresponding to the center wavelength ofeach channel. More specifically, as previously described, θ indicatesthe small tilt angle of the optical axis of input light (see FIG. 8).

[0150] Therefore, all of the wavelength components corresponding to thecenter wavelengths will have the same output angle from VIPA 240 andthus the same focusing position on mirror 254, if t is set so that, forthe wavelength component corresponding to the center wavelength in eachchannel, 2nt cos θ is an integer multiple of the center wavelength ofeach channel for the same θ and different integer.

[0151] For example, a 2 mm physical length in round trip (which isapproximately double a 1 mm thickness of VIPA 240) and a refractiveindex of 1.5 enable all the wavelengths with a spacing of 100 GHz tosatisfy this condition. As a result, VIPA 240 can compensate fordispersion in all the channels of a wavelength division multiplexedlight at the same time.

[0152] Therefore, referring to FIG. 14, with the thickness t set to theWDM matching FSR thickness, VIPA 240 and focusing lens 252 will cause(a) the wavelength component corresponding to the center wavelength ofeach channel to be focused at point 270 on mirror 254, (b) thewavelength component corresponding to the longer wavelength component ofeach channel to be focused at point 272 on mirror 254, and (c) thewavelength component corresponding to the shorter wavelength componentof each channel to be focused at point 274 on mirror 254. Therefore,VIPA 240 can be used to compensate for chromatic dispersion in allchannels of a wavelength division multiplexed light.

[0153]FIG. 16 is a graph illustrating the amount of dispersion ofseveral channels of a wavelength division multiplexed light, in a casewhen the thickness t is set to the WDM matching FSR thickness. Asillustrated in FIG. 16, all the channels are provided with the samedispersion. However, the dispersions are not continuous between thechannels. Moreover, the wavelength range for each channel at which VIPA240 will compensate for dispersion can be set by appropriately settingthe size of mirror 254.

[0154] If the thickness t is not set to the WDM matching FSR thickness,different channels of a wavelength division multiplexed light will befocused at different points on mirror 254. For example, if the thicknesst is one-half, one-third or some other fraction of the round tripoptical length thickness, then focusing points of two, three, four ormore channels may be focused on the same mirror, with each channel beingfocused at a different focusing point. More specifically, when thethickness t is one-half the WDM matching FSR thickness, the light fromodd channels will focus at the same points on mirror 254, and the lightfrom even channels will focus at the same points on mirror 254. However,the lights from the even channels will be focused at different pointsfrom the odd channels.

[0155] For example, FIG. 17 is a diagram illustrating different channelsbeing focused at different points on mirror 254. As illustrated in FIG.17, wavelength components of the center wavelength of even channels arefocused at one point on mirror 254, and wavelength components of thecenter wavelength of odd channels are focused at a different point. As aresult, VIPA 240 can adequately compensate for dispersion in all thechannels of a wavelength division multiplexed light at the same time.

[0156] There are several different ways to vary the value of thedispersion added by a VIPA. For example, FIG. 18 is a diagramillustrating a side view of an apparatus which uses a VIPA to providevariable dispersion to light. Referring now to FIG. 18, VIPA 240 causeseach different interference order to have a different angulardispersion. Therefore, the amount of dispersion added to an opticalsignal can be varied by rotating or moving VIPA 240 so that lightcorresponding to a different interference order is focused on mirror 254and reflected back into VIPA 240.

[0157]FIG. 19 is a diagram illustrating a side view of an apparatuswhich uses a VIPA to provide variable dispersion. Referring now to FIG.19, the relative distance between focusing lens 252 and mirror 254 ismaintained constant, and focusing lens 252 and mirror 254 are movedtogether relative to VIPA 240. This movement of focusing lens 252 andmirror 254 changes the shift of light returning to VIPA 240 from mirror254, and thereby varies the dispersion.

[0158] FIGS. 20(A) and 20(B) are diagrams illustrating side views ofapparatuses which use a VIPA to provide various values of chromaticdispersion to light. FIGS. 20(A) and 20(B) are similar to FIG. 14, inthat FIGS. 20(A) and 20(B) illustrate the travel directions of a longerwavelength 264, a center wavelength 266 and a shorter wavelength 268 oflight emitted by a virtual image 260 of beam waist 262.

[0159] Referring now to FIG. 20(A), mirror 254 is a convex mirror. Witha convex mirror, the beam shift is magnified. Therefore, a largechromatic dispersion can be obtained with a short lens focal length anda small amount of space. When mirror 254 is convex, as in FIG. 20(A),the convex shape can typically only be seen from a side view and cannotbe seen when viewed from the top.

[0160] Referring now to FIG. 20(B), mirror 254 is a concave mirror. Witha concave mirror, the sign of the dispersion is inverted. Therefore,anomalous dispersion can be obtained with a short lens focal length anda small space. When mirror 254 is concave, as in FIG. 20(B), the concaveshape can typically only be seen from a side view and cannot be seenwhen viewed from the top.

[0161] Therefore, typically, mirror 254 would appear flat in the topview. However, it is possible for mirror 254 to also be a concave or aconvex mirror when viewed by the top, thereby indicating that the mirroris a one-dimensional mirror.

[0162] In FIGS. 20(A) and 20(B), mirror 254 is located at or near thefocal point of focusing lens 252.

[0163] Therefore, as described above, mirror 254 can be convex orconcave in the side view, as illustrated, for example, in FIGS. 20(A)and 20(B), respectively. A convex mirror can enhance the chromaticdispersion and a concave mirror can reduce or even invert the chromaticdispersion from negative (normal) to positive (anomalous). Morespecifically, a convex mirror generates larger dispersion in thenegative direction and a concave mirror generates smaller dispersion inthe negative direction or dispersion inverted to positive. This ispossible because the magnitude of chromatic dispersion is a function ofthe curvature of the mirror in the side view.

[0164]FIG. 21 is a graph illustrating the output angle of a luminousflux from VIPA 240 versus wavelength of the luminous flux. As can beseen from FIG. 21, a curve 282 of the wavelength versus the output angleis not linear.

[0165] Since the relationship between the wavelength and the outputangle of a luminous flux produced by a VIPA is not linear, the chromaticdispersion is not constant in a wavelength band as long as a flatmirror, a normal convex mirror or a normal concave mirror is used asmirror 254. This nonlinearity in chromatic dispersion is referred to asthe higher order dispersion.

[0166] Generally, referring to the apparatuses in FIGS. 20(A) and 20(B),the nonlinearity in chromatic dispersion can be understood by referringto the following Equation (3):

(angular dispersion)·(1−f·(1/R))∞chromatic dispersion,

[0167] where f is the focal length of lens 252 and R is the radius ofcurvature of mirror 254.

[0168]FIG. 22 is a graph illustrating the angular dispersion of VIPA 240versus the wavelength of a luminous flux. Generally, the curve 284 inFIG. 22 represents the slope of curve 282 in FIG. 21. As can be seenfrom FIG. 22, the angular dispersion is not constant. Instead, theangular dispersion changes as the wavelength changes.

[0169]FIG. 23 is a graph illustrating the term (1−f·(1/R)) in Equation3, above, versus wavelength. More specifically, line 286 represents agraph of the term (1−f·(1/R)) versus wavelength for a flat mirror(radius of curvature equals “∞” (infinity)). Line 288 represents a graphof the term (1−f·(1/R)) versus wavelength for a concave mirror (radiusof curvature equals “+”). Line 290 represents a graph of the term(1−f·(1/R)) versus wavelength for convex mirror (radius of curvatureequals “−”). As illustrated in FIG. 23, each of the mirrors has aconstant radius of curvature.

[0170]FIG. 24 is a diagram illustrating the chromatic dispersion versuswavelength of an apparatus such as in FIGS. 20(A) and 20(B), when mirror254 is a convex mirror, a flat mirror and a concave mirror. Morespecifically, curve 292 is a curve of the chromatic dispersion versuswavelength when mirror 254 is a convex mirror. Curve 294 is a curve ofthe chromatic dispersion versus wavelength when mirror 254 is a flatmirror. Curve 296 is a curve, of the chromatic dispersion versuswavelength when mirror 254 is a concave mirror.

[0171] In a very general manner, curves 292, 294 and 296 each representa product of the angular dispersion illustrated in FIG. 22 with theappropriate line illustrated in FIG. 23, as indicated by Equation 3,above. More specifically, generally, curve 292 represents a product ofcurve 284 in FIG. 22 and line 290 in FIG. 23. Generally, curve 294represents a product of curve 284 in FIG. 22 and line 286 in FIG. 23.Generally, curve 296 represents a product of curve 284 in FIG. 22 andline 288 in FIG. 23.

[0172] As can be seen from FIG. 24, the chromatic dispersion is notconstant whether a convex, flat or concave mirror is used as mirror 254.

[0173] According to the above, this wavelength dependence of chromaticdispersion can be reduced or eliminated by chirping the curvature ofmirror 254.

[0174] More specifically, FIG. 25 is a graph illustrating a curve 298 ofthe term (1−f·(1/R)) in Equation 3, above, versus wavelength. Generally,curve 298 in FIG. 25 is inverse to curve 284 in FIG. 22. Therefore, amirror having the characteristics in FIG. 25 will provide a constantchromatic dispersion, as illustrated by the curve 300 in FIG. 26.

[0175] For example, with the apparatus illustrated, for example, in FIG.14, a longer wavelength has a larger dispersion in the negativedirection than a shorter wavelength. Therefore, mirror 254 can bedesigned to have a concave portion where the longer wavelength reflects,and a convex portion were the shorter wavelength reflects, toeffectively cancel the wavelength dependence of dispersion. Ideally, thecurvature of mirror 254 varies from convex to concave continuously alongthe focusing point of light when the wavelength changes from short tolong. If this modification is based on a conventional convex mirror, nota flat mirror, the curvature of the mirror can be made to vary fromstrong convex to weak convex continuously along the focusing point oflight when the wavelength changes from short to long.

[0176] Therefore, there are many different designs for mirror 254, toprovide a constant chromatic dispersion. For example, FIG. 27 is a graphillustrating characteristics many different mirror designs. Curve 302 inFIG. 27 illustrates a mirror which continuously changes from convex toconcave as the wavelength of output light increases. Curve 304illustrates a mirror which changes from strongly convex to slightlyconvex as the wavelength of output light increases. Curve 306illustrates a mirror which changes from slightly concave to stronglyconcave as the wavelength of output light increases. Other mirrordesigns include, for example, those shown by curves 308 and 310.

[0177] There are a virtually unlimited number of mirror designs whichcould be used, and such designs could be graphed in FIG. 27. Moreover,mirror designs are not limited to those having characteristic curveswith the same slopes as those in FIG. 27.

[0178] FIGS. 28(A), 28(B), 28(C) and 28(D) illustrate the surface shapeof various mirrors which can be used as mirror 254. For example, FIG.28(A) illustrates a mirror which continuously changes from convex toconcave, as represented by curve 302 in FIG. 27. FIG. 28(B) illustratesa mirror which continuously changes from strong convex to weak convex,as represented by curve 310 in FIG. 27. FIG. 28(C) illustrates a mirrorwhich continuously changes from weak concave to strong concave, asrepresented by curve 306 in FIG. 27.

[0179] Moreover, there are a virtually unlimited number of mirrordesigns which could be used. For example, FIG. 28(D) illustrates a flatmirror which changes to convex. FIG. 27(E) illustrates a flat mirrorwhich changes to concave. FIG. 28(F) illustrates a mirror having aconvex portion and a concave portion, but where the mirror does notcontinuously change from convex to concave.

[0180] Therefore, as indicated above, an apparatus includes a VIPA, amirror and a lens. The VIPA receives an input light and produces acorresponding output light (such as a luminous flux) propagating awayfrom the VIPA. The lens focuses the output light onto the mirror so thatthe mirror reflects the output light and the reflected light is directedby the lens back to the VIPA. The mirror has a shape which causes theapparatus to produce a constant chromatic dispersion.

[0181] For example, output light focused by the lens is incident on adifferent surface point on the mirror as the wavelength of the outputlight changes. The mirror is shaped so that the surface points changecontinuously from convex to concave as the wavelength of the outputlight changes from shorter to longer. As another example, the mirror canbe shaped so that the surface points change continuously from strongerconvex to weaker convex as the wavelength of the output light changesfrom shorter to longer.

[0182] Alternatively, the mirror can be shaped so that the surfacepoints change continuously from weaker concave to stronger concave asthe wavelength of the output light changes from shorter to longer. Thereare many other examples. For example, the mirror can have a concaveportion and a convex portion so that output light at a shorterwavelength than a specific wavelength reflects off the convex portionand so that output light at a longer wavelength than the specificwavelength reflect off the concave portion.

[0183] Moreover, for example, the mirror can have a flat portion whichcontinuously changes to a concave portion in correspondence with anincrease in the wavelength of the output light above a specificwavelength so that output light at a shorter wavelength than thespecific wavelength is incident on the flat portion and output light ata longer wavelength than the specific wavelength is incident on theconcave portion. Or, the mirror can have a convex portion whichcontinuously changes to a flat portion in corresponding with an increasein the wavelength of the output light above a specific wavelength sothat output light at a shorter wavelength than the specific Wavelengthis incident on the convex portion and output light at a longerwavelength than the specific wavelength is incident on the flat portion.

[0184] A VIPA, as described above, provides a much larger angulardispersion than a diffraction grating. Therefore, a VIPA can be used tocompensate for much larger chromatic dispersion than a spatial gratingpair arrangement as illustrated in FIGS. 6(A) and 6(B).

[0185] A mirror, as described above, to reflect light back to a VIPA tocompensate for chromatic dispersion, can be described as a cylindricalmirror since the mirror shape is that of the surface of a cylinder. Inother words, as shown in FIG. 29, the mirror has the same radius ofcurvature along an axis forming the cylinder. Since chromatic dispersionis a function of the radius of the mirror curvature as described above,the chromatic dispersion will not change when the mirror is moved alongthe axis forming the cylinder. As shown in FIG. 30(A), the chromaticdispersion may change within each channel as previously described (seeFIG. 24). However, the chromatic dispersion will be periodic, as shownin FIG. 30(B), and the chromatic dispersion will be approximately thesame for all the channels.

[0186]FIG. 31(A) is a graph illustrating chromatic dispersion versuswavelength for one channel of a wavelength division multiplexed light,after undergoing chromatic dispersion compensation with a VIPA with amodified cylindrical mirror as in, for example, FIGS. 28(A) through28(F). Referring now to FIG. 31(A), it can be seen that the amount ofchromatic dispersion is substantially the same for each wavelengthwithin the same channel.

[0187]FIG. 31(B) is a graph illustrating chromatic dispersion versuswavelength for all wavelengths (and therefore, many channels) of awavelength division multiplexed light, after undergoing chromaticdispersion compensation with a VIPA with a modified cylindrical mirroras in, for example, FIGS. 28(A) through 28(F). Referring now to FIG.31(B), it can be seen that the amount of chromatic dispersion issubstantially the same, or uniform, for all wavelengths in all channels.

[0188]FIG. 32 is a diagram illustrating a top view of an apparatus usinga VIPA to provide variable chromatic dispersion to light, according to aher embodiment of the present invention. Referring now to FIG. 32, acone shaped mirror 400 is used to reflect light back to VIPA 240. Mirror400 is movable in a direction 401.

[0189] As previously indicated, VIPA 240 produces a collimated luminousflux, which can be referred to as a collimated output light, travelingin a direction determined by the wavelength of the light. The angulardispersion direction of VIPA 240 is the direction in which the travelingdirection of the collimated output light changes as the wavelength ofthe light changes, and is represented, for example, by direction 402 inFIG. 32. Collimated output lights for different wavelengths will be inthe same plane.

[0190] Therefore, direction 401 is along the surface of the cone and canbe described as being perpendicular to both the angular dispersiondirection of VIPA 240 and the traveling directions of collimated lightfrom VIPA 240. Alternatively, direction 401 can be described as beingperpendicular to a plane which includes the traveling direction of thecollimated output lights for different wavelengths from VIPA 240.

[0191] FIGS. 33(A) and 33(B) are diagrams illustrating how mirror 400can be formed, for example, from a section of a cone 405, according toan embodiment of the present invention. As can be seen from FIG. 33(A),direction 401 preferably passes along the surface of, and through thetop of, cone 405. Although it is preferable for direction 401 to passthrough the top of cone 405, it is not necessary to pass through thetop.

[0192] In FIG. 33(B), mirror 400 is shown with three different radii ofcurvature A, B and C. Radius of curvature A is the largest, radius ofcurvature C is the smallest, and radius of curvature B is between A andC in size.

[0193] By moving the mirror in direction 401 (corresponding, forexample, to direction 401 in FIG. 32), the position of the light focusmoves from A to C on the surface of the cone shaped mirror in FIG.33(B). Since the radii are different for A, B and C, the chromaticdispersion will be different. Thus, the chromatic dispersion will bevaried by moving the cone shaped mirror.

[0194]FIG. 34(A) is a graph illustrating the amount of chromaticdispersion versus wavelength within one channel for radii of curvatureA, B and C of a cone shaped mirror when the mirror is moved in adirection such as direction 401, according to an embodiment of thepresent invention. As can be seen from FIG. 34(A), generally, radius ofcurvature C produces the greatest amount of chromatic dispersion.Generally, radius of curvature A produces the smallest amount ofchromatic dispersion. As can be seen from FIG. 34(A), the amount ofchromatic dispersion produced by radius of curvature B is between A andC.

[0195] As can be seen from FIG. 34(A) and also described with referenceto FIGS. 24 and 30(A), the amount of chromatic dispersion will bedifferent for different wavelengths within a channel. However, asdescribed with reference to FIGS. 26, 31(A) and 31(B), by modifying themirror, it is possible to provide a uniform amount of chromaticdispersion in each channel, and in all the channels.

[0196] For example, FIG. 34(B) is a diagram illustrating the radii ofcurvature A, B and C when a cone shaped mirror is moved in a directionsuch as direction 401, according to an embodiment of the presentinvention. By contrast, FIG. 34(C) is a diagram illustrating modifiedradii of curvature A′, B′ and C′ when a modified cone shaped mirror toprovide uniform chromatic dispersion is moved in a direction such asdirection 401, according to an embodiment of the present invention. Forexample, in the modified mirror, output light focused by lens 252 isincident on a different surface point on the mirror as the wavelength ofthe output light changes. The mirror is shaped so that the surfacepoints change continuously from convex to concave as the wavelength ofthe output light changes from shorter to longer. As another example, themirror can be shaped so that the surface points change continuously fromstronger convex to weaker convex as the wavelength of the output lightchanges from shorter to longer.

[0197] Alternatively, the mirror can be shaped so that the surfacepoints change continuously from weaker concave to stronger concave asthe wavelength of the output light changes from shorter to longer. Thereare many other examples. For example, the mirror can have a concaveportion and a convex portion so that output light at a shorterwavelength than a specific wavelength reflects off the convex portionand so that output light at a longer wavelength than the specificwavelength reflect off the concave portion.

[0198] As a result, the modified mirror will provide a uniform chromaticdispersion in each channel, and in all the channels.

[0199]FIG. 35 is a graph illustrating the chromatic dispersion versuswavelength in one channel for radii of curvature A′, B′ and C′,according to an embodiment of the present invention. As can be seen fromFIG. 35, each radii of curvature A′, B′ and C′ produces a uniform butdifferent amount of chromatic dispersion. Therefore, each channel willhave a uniform chromatic dispersion and the amount of the chromaticdispersion is variable by moving the mirror.

[0200]FIG. 36 is a diagram illustrating various angles in an apparatuswhich uses a VIPA, according to an embodiment of the present invention.Referring now to FIG. 36, Θ and θ are the average incident angles, and Φand φ are the output angles with respect to the normal line to a plate,such as second surface 244, forming VIPA 240. Θ and Φ indicate theangles in air, whereas θ and φ indicate the angles in glass betweensurfaces 242 and 244 of VIPA 240. The angles in the air areapproximately n times larger than those in the glass because of therefraction at the glass surface. Here, n is the index of the glass.

[0201]FIG. 37 is an additional diagram illustrating angles in anapparatus which uses a VIPA, according to an embodiment of the presentinvention. As indicated in FIG. 37, the output angle φ is determined asthe direction where the difference in the light paths originating at twoadjacent beam waists is a multiple of the light wavelength. The spacingbetween the adjacent beam waists is 2t (t is the thickness of the VIPA,as illustrated, for example, in FIG. 8) and the output angle in theglass is φ. So, 2t cos φ=mλ/n (m is an integer). From this, the angulardispersion is dΦ/dλ=−n²/λΦ, as shown by the following Equation (4):$\begin{matrix}{{{\text{Separation~~of~~the~~light~~paths:}\quad d} = {2t\quad \sin \quad \varphi}}{{\text{Difference~~of~~the~~path~~lengths:}\quad {m \cdot \frac{\lambda}{n}}} = {{2t\quad \cos \quad \varphi \quad \frac{m\quad \Delta \quad \lambda}{n}} = {{{- 2}t\quad \sin \quad {\varphi\Delta\varphi}{\Delta \quad \varphi}} = {{{- \cot}\quad {\varphi \cdot \frac{\Delta \quad \lambda}{\lambda}}} \approx {{- \frac{1}{\varphi}}\frac{\Delta \quad \lambda}{\lambda}}}}}}{\theta:\text{Input~~angle~~in~~glass}}{\varphi:\text{Output~~angle~~in~~glass}}{\Theta:\text{Input~~angle~~in~~air}}\quad {\Phi:\text{Output~~angle~~in~~air}}\quad {\Theta \approx {n\quad \theta}}\quad {\Phi \approx \quad {n\quad \varphi}}\quad {{{\Delta \quad \Phi} \approx {\Delta \quad \varphi {\Delta\Phi}} \approx {{- \frac{n}{\varphi}}\frac{\Delta \quad \lambda}{\lambda}} \approx {{- \quad \frac{n^{2}}{\Phi}}\frac{\Delta \quad \lambda}{\lambda}}},{\frac{\Phi}{\lambda} \approx {- \frac{n^{2}}{\lambda \quad \Phi}}}}} & {{Equation}\quad (4)}\end{matrix}$

[0202]FIG. 38 is a diagram illustrating how chromatic dispersion isgenerated in an apparatus using a VIPA, according to an embodiment ofthe present invention. FIG. 14 also illustrates how chromatic dispersionis generated, but FIG. 38 is a more quantitative description.

[0203] Referring now to FIG. 38, the light travel angle in the air withrespect to the normal line to the VIPA is Φ-Θ. Also, the focal length oflens 252 is f and the depth of the center beam waist is a. The lightfocusing position y on the mirror is y=f(Φ-Θ). The mirror shape is c(y)as a function of y. The mirror slope h is dc/dy. Then, the beam shiftafter the round trip is obtained by the following Equation (5):$\begin{matrix}{{{\text{Mirror~~shape:}{c(y)}},\text{Slope~~of~~mirror~~surface:}}{{{h(y)} = \frac{{c(y)}}{y}},{y \approx {f\left( {\Phi - \Theta} \right)}}}{\text{(Beam~~shift)} \approx {{2\left( {f - a} \right)\left( {\Phi - \Theta} \right)} + {2f\quad {h(y)}}}}{\text{(Delay)} = {{\frac{n}{c}\left( {{Distance}\quad {change}} \right)} \approx {\frac{n}{c} \cdot \frac{\text{(Beam~~shift)}}{\varphi}}\quad \approx {\frac{2n^{2}}{c\quad \Phi}\left\{ {{\left( {f - a} \right)\left( {\Phi - \Theta} \right)} + {{fh}(y)}} \right\}}}}} & {{Equation}\quad (5)}\end{matrix}$

[0204] The distance change in FIG. 38 is easily obtained from the beamshift, and the delay is the distance change divided by the speed oflight in the glass. The chromatic dispersion is calculated as the delaychange with the wavelength change and is shown by the following Equation(6): $\begin{matrix}\begin{matrix}{\text{(Dispersion)} = \frac{({Delay})}{\lambda}} \\{\approx {\frac{2n^{2}}{c\quad \Phi}\left\{ {\left( {f - a} \right) + {f\frac{{h(y)}}{y}\frac{y}{\Phi}}} \right\} \frac{\Phi}{\lambda}}} \\{\approx {{- \frac{2n^{4}}{c\quad {\lambda\Phi}^{2}}}\left\{ {\left( {f - a} \right) + {f^{2}\frac{{h(y)}}{y}}} \right\}}}\end{matrix} & {{Equation}\quad (6)}\end{matrix}$

[0205] If the mirror is a cylindrical mirror and has a circular shapealong with angular dispersion direction, dh/dy is simply 1/r and thefollowing Equation (7) is obtained: $\begin{matrix}{\text{For~~a~~cylindrical~~mirror~~of~~radius}\quad {r:\left( {\text{Dispersion)} \approx {{- \frac{2n^{4}}{c\quad {\lambda\Phi}^{2}}}\left\{ {f - a + \frac{f^{2}}{r}} \right\}}} \right.}} & {{Equation}\quad (7)}\end{matrix}$

[0206] From Equation (7), it can be seen that chromatic dispersion isnot uniform in a WDM channel and, instead, the chromatic dispersionchanges approximately in proportion to 1/Φ².

[0207] As indicated in Equation (6), chromatic dispersion is a functionof Φ. To make this dispersion uniform in a WDM channel, this formulaneeds to be constant as Φ changes. Therefore, the value in the largeparenthesis of Equation (6) should be proportional to Φ² (small changeof λ is ignored). Assuming the proportional constant is K (this meansthe chromatic dispersion is −2n⁴K/cλ) and that n, c, λ, f and a areconstant or almost constant for the sell change of wavelength, we getthe following Equation (8). $\begin{matrix}{{{\left( {f - a} \right) + {f^{2}\frac{{h(y)}}{y}\quad \text{is~~~proportional~~~to}\quad {\Phi^{2}.\text{Here,}}\quad y}} \approx {{f\left( {\Phi - \Theta} \right)}.\quad {So}}},{\Phi^{2} = {{\frac{1}{f^{2}}y^{2}} + {\frac{2\Theta}{f}y} + {\Theta^{2}\text{The~~condition~~for~~a~~uniform~~dispersion~~in~~a}{{WDM}\quad \text{channel~~is}}{{\left( {f - a} \right) + {f^{2}\frac{{h(y)}}{y}}} = {{\frac{K}{f^{2}}y^{2}} + {\frac{2K\quad \Theta}{f}y} + {K\quad \Theta^{2}}}}{\frac{{h(y)}}{y} = {\frac{1}{f^{2}}\left\{ {{\frac{K}{f^{2}}y^{2}} + {\frac{2K\quad \Theta}{f}y} + {K\quad \Theta^{2}} - f + a} \right\}}}}}}} & {{Equation}\quad (8)}\end{matrix}$

[0208] The mirror slope h should be zero at the center y=0. Equation (8)is integrated to get the following Equation (9): $\begin{matrix}{{h(y)} = {{\int_{0}^{y}{\left( {{\frac{K}{f^{4}}y^{2}} + {\frac{2K\quad \Theta}{f^{3}}y} + \frac{{K\quad \Theta^{2}} - f + a}{f^{2}}} \right)\quad {y}}}\quad = {{\frac{K}{3f^{4}}y^{3}} + {\frac{K\quad \Theta}{f^{3}}y^{2}} + {\frac{{K\quad \Theta^{2}} - f + a}{f^{2}}y}}}} & {{Equation}\quad (9)}\end{matrix}$

[0209] The mirror curve is obtained after another integration and isshown by the following Equation (10): $\begin{matrix}{{c(y)} = {{\int{{h(y)}{y}}}\quad = {{\frac{K}{12f^{4}}y^{4}} + {\frac{K\quad \Theta}{3f^{3}}y^{3}} + {\frac{{K\quad \Theta^{2}} - f + a}{2f^{2}}y^{2}}}}} & {{Equation}\quad (10)}\end{matrix}$

[0210] Equation (10) determines the ideal curves for different K, whichwere described, for example, in FIG. 28.

[0211] The mirror shape is determined by the value K, which gives thechromatic dispersion. To get the shape along the curve A, B, and C inFIG. 33(B), a small K, a medium K, and a large K can be used,respectively, for Equation (10). The curves are illustrated in FIGS.39(A), 39(B) and 39(C). However, for easy manufacturing, the shapescould be approximately a part of an ellipse, or a parabola, or ahyperbola. In these cases, the mirror can be made as a part of a cone.

[0212]FIG. 40 is a diagram illustrating an example of a cone for forminga mirror, according to an embodiment of the present invention. Referringnow to FIG. 40, cone 405 has a base 406. If base 406 is a circle, cone405 is a normal cone. However, cone 405 may be stretched, for example,in a side direction. In such case, base 406 will be ellipse, as shown inFIG. 40. In the case of ellipse, base 406 has a longer axis r₁ and ashorter axis r₂. Direction 401 is determined by the line passing alongthe cone surface from the top of the cone to the bottom where the conesurface hits the longer or shorter axis in base 406. However, this linedoes not necessarily lave to hit one of the axes. As shown in FIG. 40,cone 406 is cut by a plane 407 which is perpendicular to direction 401.A cut curve 408 for the mirror is an ellipse, parabola or hyperbola,depending on the top angle of cone 405. Therefore, cut curve 408 in themirror area is a part of one of these three curves. A modified coneshaped mirror is defined so that cut curve 408 is determined by Equation(10), rather than the three shapes.

[0213] Light for different WDM channels will be focused at differentpositions displaced in the direction 401. Therefore, the different WDMchannels will see different curves and generate different chromaticdispersion. Therefore, the cone shape can be further modified so thatthe cut curves for different WDM channels are determined by Equation(10) with desirable value Ks. This indicates that the dispersion changeis not limited to a linear change with wavelength or WDM channels and itcould change in any way.

[0214]FIG. 41 is a diagram illustrating a step shaped mirror surface,according to an embodiment of the present invention. This mirror canprovide different shapes for different WDM channels without causing anexcess tilt of the mirror with respect to the incident light.

[0215] Referring again to FIG. 32, mirror 400 is movable in direction401. Mirror 400 can also be described as movable in or around a focalplane of lens 252. Mirror 400 has a cone shape, or modified cone shape,as described above, so mirror 400 will have different curvatures alongthe surface. Since the curvature changes along direction 401, and mirror400 is movable in this direction, the chromatic dispersion can be variedby moving mirror 400 by a relatively small distance. In this design, themoving distance of mirror 400 would typically be less than 1 cm, whichis much smaller tan the moving distance of mirror 254 in FIG. 19.

[0216] Further, in FIG. 19, the position of lens 252 is movable, whereasin FIG. 32, the position of lens 252 would typically be fixed.Therefore, in FIG. 19, a large space will be required between VIPA 240and lens 252, so that the lens 252 and mirror 254 can be moved togetherfor a relatively large distance to provide the required amount ofchromatic dispersion. This large space between VIPA 240 and lens 252 isundesirable, and greatly increases the overall size of the apparatus. Bycomparison, in FIG. 32, a relatively small space is required betweenVIPA 240 and lens 252, and mirror 400 only has to move a relativelysmall distance to provide the required amount of chromatic dispersion,thereby allowing the overall apparatus to be much smaller than that inFIG. 19.

[0217]FIG. 42 is a diagram illustrating a side view of an apparatususing a VIPA to provide chromatic dispersion slope, according to anadditional embodiment of the present invention. Referring now to FIG.42, an angular dispersive component 500 is positioned between VIPA 240and lens 252. Angular dispersive component 500 could be, for example, atransmission type diffraction grating, a reflection type diffractiongrating or a holographic grating.

[0218] Angular dispersive component 500 has an angular dispersiondirection which is perpendicular to the angular dispersion direction ofVIPA 240.

[0219] Preferably, the amount of angular dispersion provided by angulardispersive component 500 should be large enough to distinguish thedifferent wavelengths for different WDM channels. Therefore, preferably,the angular dispersion provided by angular dispersive component 500should be larger than approximately 0.1 degrees/nm. This number isreadily achievable by using a diffraction grating as angular dispersivecomponent 500. However, the present invention is not limited to anyparticular amount of angular dispersion.

[0220] In FIG. 42, the position of mirror 400 is preferably fixed. Thisis different than in FIG. 32, where the position of mirror 400 ismovable. However, in FIG. 42, mirror 400 is not limited to being fixed,and can be movable to add variable dispersion.

[0221] By using angular dispersive component 500 between VIPA 240 andlens 252, the light in different channels will be focused by lens 252 atpositions which are displaced along direction 401 (not shown in FIG. 42)on the surface of mirror 400 because of the angular dispersion ofangular dispersive component 500, and will see a different curvature ofmirror 400. As a result, different channels will have differentchromatic dispersions. This channel dependent chromatic dispersion iscalled high order dispersion or dispersion slope, and is required forcompensation of a fiber dispersion since different WDM channelstraveling in a fiber will see different chromatic dispersion in thefiber.

[0222]FIG. 43(A) is a graph illustrating the amount of chromaticdispersion for all wavelengths (many channels) with a cone shaped mirrorused as mirror 400 in FIG. 42, according to an embodiment of the presentinvention. For example, this cone shaped mirror would typically be asillustrated in FIGS. 33(A) and 33(B). As illustrated in FIG. 43(A), theamount of chromatic dispersion is not uniform in each channel anddiffers for different channels.

[0223]FIG. 43(B) is a graph illustrating the amount of chromaticdispersion for all wavelengths (many channels) with a modified coneshaped mirror used as mirror 400 in FIG. 42, according to an embodimentof the present invention. For example, this modified cone shaped mirrorwould typically have radii of curvature A′, B′ and C′ as in FIG. 34(C),according to an embodiment of the present invention. As illustrated inFIG. 43(B), the amount of chromatic dispersion is uniform in eachchannel and different for different channels.

[0224] In FIGS. 43(A) and 43(B), the dispersion is shown as increasingwith increasing wavelength. However, in some embodiments of the presentinvention, the dispersion could decrease with increasing wavelength byinverting angular dispersive component 500 or by inverting the directionof the cone shaped mirror.

[0225] Therefore, parameters (such as the mirror shape, lens focallength, etc.) are preferably designed so that the chromatic dispersionfor each WDM channel, such as those shown, for example, in FIGS. 43(A)or 43(B), is the same amount but opposite sign to the chromaticdispersion of the transmission line at the corresponding wavelength forthe purpose of the simultaneous dispersion compensation of all WDMchannels. Namely, although different WDM channels may experiencedifferent chromatic dispersion amounts through the transmission line, aVIPA can be used, as described herein, to compensate for the dispersionof the WDM channels with different dispersion amounts.

[0226]FIG. 44 is a diagram illustrating the use of a holographic grating510 as an angular dispersive component between VIPA 240 and lens 252,according to an embodiment of the present invention.

[0227] Moreover, FIG. 45 is a diagram illustrating the use of areflection type grating 520 as an angular dispersive component betweenVIPA 240 and lens 252, according to an embodiment of the presentinvention.

[0228] When a diffraction grating is used as an angular dispersivecomponent (see FIG. 42), one problem is its polarization dependence.Therefore, a quarter wave plate can be used to cancel the polarizationdependence of the diffraction grating.

[0229] For example, FIG. 46 is a diagram illustrating the use of aquarter wave plate 530 inserted between the diffraction grating and lens252.

[0230]FIG. 47 is a diagram illustrating the use of quarter wave plate530 inserted between lens 252 and the cone shape mirror 400. As anexample, quarter wave plate 530 is positioned with the axes at 45° withrespect to the plane of s or p polarization of the diffraction grating.

[0231] With configurations as in FIGS. 46 and 47, light passed throughthe diffraction grating with p-polarization will return to thediffraction grating with s-polarization, and light passed through thediffraction grating with s-polarization will return to the diffractiongrating with p-polarization. Therefore, the polarization dependence ofthe diffraction grating is canceled.

[0232]FIG. 48(A) is a diagram illustrating a side or top view of anapparatus which uses a VIPA to provide two different chromaticdispersions for different channels, according to a still furtherembodiment of the present invention. Referring now to FIG. 48(A), awavelength filter 510 is positioned between lens 252 and mirrors M1 andM2. Wavelength filter 510 filters the light from lens 252 so that lightat wavelength λ1 is directed to mirror M1, and light at wavelength λ2 isdirected to mirror M2. Mirror M1 has a different curvature than mirrorM2 and therefore, λ1 and λ2 will have different chromatic dispersion.Thus, each of mirrors M1 and M2 can be, for example, a cylindricalmirror or a modified cylindrical mirror, as described herein. Forexample, mirrors M1 and M2 can be modified cylindrical mirrors toprovide uniform but different amount of chromatic dispersion in channelscorresponding to λ1 and λ2.

[0233]FIG. 48(B) is a graph illustrating chromatic dispersion versuswavelength for the apparatus in FIG. 48(A), where mirrors M1 and M2 aremodified cylindrical mirrors to provide uniform chromatic dispersionwithin each channel, according to an embodiment of the presentinvention.

[0234] While FIG. 48(A) shows an apparatus configured for twowavelengths, there is generally no limit in the number of wavelengthfilters and mirrors which can be used to separate additional wavelengthsor channels.

[0235] For example, FIG. 49 is a diagram illustrating a side or top viewof an apparatus which uses a VIPA to provide three different chromaticdispersion for different channels, according to an embodiment of thepresent invention. Referring now to FIG. 49, wavelength filters 520 and530 are used to direct light at wavelengths λ1, λ2 and λ3 to mirrors M1,M2 and M3, respectively.

[0236] According to the above embodiments of the present invention, anapparatus which uses a VIPA in combination with a mirror, such as a coneor modified cone shaped mirror, to generate dispersion slope or higherorder dispersion. The cone or modified cone shape of the mirror isdesigned so that the dispersion slope or higher order dispersion of theapparatus compensates for dispersion slope or higher order dispersion ofa transmission line (fiber).

[0237] In an optical communication system in which a transmittertransmits an optical signal through a transmission line to a receiver,the apparatus of the present invention can be inserted in thetransmitter, the transmission line, the receiver, or in any combinationof the transmitter, transmission line and receiver. For example, in FIG.1, the apparatus of the present invention can be inserted in transmitter30, optical fiber 34 (for example, a transmission line) or receiver 36,or in any combination of transmitter 30, optical fiber 34 and receiver36. Further, two or more of the apparatuses of the present invention canbe cascaded together, or only one apparatus can be used in transmitter30, optical fiber 34 and/or receiver 36. Thus, the present invention isnot limited to the number of apparatuses which can be used together toprovide the required affect.

[0238] One problem with an apparatus which use a VIPA to providechromatic dispersion, as in the above-described embodiments of thepresent invention, is that the apparatus has a relatively narrow band inthe transmission spectrum. Generally, the band is narrow due toinsertion loss from fiber-to-fiber. For example, in FIG. 13, insertionloss occurs from the light traveling out of fiber 246 to when the lightis again received by fiber 246 after traveling through VIPA 240 andbeing reflected by mirror 254.

[0239] For example, FIG. 50 is a graph illustrating the insertion lossin an apparatus which uses a VIPA to provide chromatic dispersion,according to an embodiment of the present invention. Referring now toFIG. 50, curve 550 illustrates the actual insertion loss which mighttypically occur for one channel. By contrast, curve 560 illustrates amore desirable insertion loss for the channel.

[0240] The insertion loss is due to several different factors, one majorfactor is a loss due to different diffraction efficiency at differentwavelengths.

[0241] For example, FIG. 51 is a diagram illustrating differentdiffraction efficiency at different wavelengths. Referring now to FIG.51, light output from VIPA 240 is focused by lens 252 on a mirror 570.Light at the shortest wavelength is focused at point 580, light at thecenter wavelength is focused at point 590, and light at the longestwavelength is focused at point 600. However, due to the characteristicsof VIPA 240, and especially to the physics underlying the multiplereflection incurring inside VIPA 240, the light at the center wavelengthat point 590 will be the strongest, whereas the light at the shortestwavelength and the longest wavelength at points 580 and 600,respectively, will be weaker.

[0242] For example, FIG. 52 is a diagram illustrating the lightintensity of light traveling out of a fiber and into a VIPA in the aboveembodiments of the present invention. FIG. 52 includes fiber 246 andlenses 248 and 250 as in FIG. 13, but the VIPA is removed and the lightis allowed to travel to a screen 610. A dotted box 240 shows where theVIPA would be positioned.

[0243] As indicated in FIG. 52, the light has a light intensity shown bycurve 620 at screen 610. As a result, the insertion loss can be madecloser to the desired insertion loss 560 in FIG. 50 if the far fielddistribution of the input light provided to the VIPA is a double-humpedshape. In this manner, the transmission spectrum of the apparatus willbe much flatter.

[0244]FIG. 53 is a diagram illustrating a side view of an optical phasemask on an input fiber to produce a double-humped shape far fielddistribution, in an apparatus which uses a VIPA to provide chromaticdispersion, according to an embodiment of the present invention.Referring now to FIG. 53, an input fiber 246 (corresponding, forexample, to input fiber 246 in FIG. 13) has a core 650. Optical phasemasks 660 and 670 cover a portion of the top and bottom, respectively,of core 650. As a result, a double-humped shape far field distributionwill be provided at the input to the VIPA (not illustrated in FIG. 53),and the insertion loss of the apparatus will have a more desirableinsertion loss.

[0245]FIG. 54 is a diagram illustrating a cross-sectional view alonglines 54-54 in FIG. 53, according to an embodiment of the presentinvention. As can be seen from FIGS. 53 and 54, phase masks 660 and 670cover the top and bottom, respectively. The phase masks should not be onthe side portions of the core.

[0246] It is not necessary for the phase masks to be on the input fiber.Instead, for example, the phase masks could be on the VIPA.

[0247] For example, FIG. 55 is a diagram illustrating a side view ofphase masks on a VIPA to provide a double-humped shape far fielddistribution with respect to light received inside the VIPA, accordingto an embodiment of the present invention. Elements in FIG. 55 aresimilar to that in FIG. 11.

[0248] Referring now to FIG. 55, optical phase masks 690 and 695 arepositioned on the light incident window surface 124, to provide adouble-humped shape far field distribution of light received into theVIPA.

[0249]FIG. 56 is a diagram illustrating a side view of phase masks on aVIPA to provide a double-humped shape far field distribution withrespect to light received inside the VIPA, according to an additionalembodiment of the present invention. FIG. 56 is different than FIG. 55in that phase masks 690 and 695 are provided on reflecting surface 122.Therefore, phase masks can be on either reflecting surface or on thelight incident window of the VIPA.

[0250] Further, a double-humped shape far field distribution can beobtained by positioning phase masks in the center of the input light.

[0251] For example, FIGS. 57 and 58 are diagrams illustrating a sideview of phase masks on a VIPA to provide a double-humped shape far fielddistribution with respect to light received inside the VIPA, accordingto an additional embodiment of the present invention. In FIGS. 57 and58, a phase mask 700 is positioned in the center of the input light. Inthis case, the optical phase at the center of the far field distributionmay be π, and may be 0 at the ends. This is the opposite of the farfield distribution in FIGS. 53-56.

[0252] As indicated above, phase masks can be used to provide adouble-humped shape far field distribution. The phase mask preferablyhas a thickness corresponding to the addition of π to the optical phase.However, a preferable range of optical phase added by the phase mask is⅔ π to {fraction (4/3)} π.

[0253] Any transparent material that provides the proper additionalphase can be used for the phase mask. For example, SiO₂ would be atypical material for use as a phase mask.

[0254] As indicated above, a phase mask is used to provide a double-humpshaped far field distribution. Here, a “double-humped shape” is definedas having two almost identical peaks with a valley between the peaks.The depth of the valley should be less than or equal to 50% of the toppeak value, and preferably less than 20% of the top peak value.Preferably, the peaks are identical, but it is satisfactory for thepeaks to have an amplitude of within 10% of each other.

[0255] Further, instead of using a phase mask, there are other ways toproduce a double-hump shaped far field distribution, and the presentinvention is not limited to using a phase mask for this purpose.

[0256] The above described embodiments using a phase mask to produce adouble-hump shaped far field distribution are applicable to embodimentsof the present invention that use a VIPA to produce chromaticdispersion. However, these embodiments are also applicable to the use ofa VIPA as a demultiplexer. For example, the above-described embodimentsof the present invention relating to the use of a phase mask to producea double-hump shaped far field distribution can be applied to the VIPAin FIGS. 7 and 8.

[0257] As described above, an apparatus using a VIPA to compensate forchromatic dispersion would typically have a loss curve in each WDMchannel as shown in FIG. 50. As described above, this loss curve can beflattened by using an optical phase mask. However, there are other waysto flatten the loss curve, such as by adding excess loss.

[0258] For example, FIG. 59 is a diagram illustrating excessive lossadded to the loss curve, according to an embodiment of the presentinvention. Referring now to FIG. 59, by adding excess loss 705, losscurve 550 will be flattened to become curve 710.

[0259]FIG. 60 is a diagram illustrating the use of an excess losscomponent to provide excess loss, and thereby flatten the loss curve,according to an embodiment of the present invention. Referring now toFIG. 60, a VIPA dispersion compensator 720 represents an apparatus whichuses a VIPA to produce chromatic dispersion, as described herein. Anexcess loss component 730 is cascaded with VIPA dispersion component720. Excess loss component 730 could be either upstream or downstream ofVIPA dispersion component 720 and there might be some optical componentsbetween VIPA dispersion component 720 and excess loss component 730.Thus, the present invention is not limited to any specific placement ofVIPA dispersion component 720 with respect to excess loss component 730.

[0260] Excess loss component 730 can be, for example, an opticalinterferometer or a wavelength filter. However, a Mach-Zehnderinterferometer or a Fabry-Perot interferometer would be suitable,because they have a periodic transmission curve and the period can beadjusted to the WDM channel spacing by choosing appropriate parametersof the interferometer. Therefore, the overall transmission curve will beflattened for all the WDM channels simultaneously.

[0261] The above described embodiments using an excess loss componentare applicable to embodiments of the present invention that use a VIPAto produce chromatic dispersion. However, these embodiments are alsoapplicable to the use of a VIPA as a demultiplexer. For example, theabove-described embodiments of the present invention relating to the useof an excess loss component can be applied with the VIPA in FIGS. 7 and8.

[0262] Instead of using an excessive loss component, there are otherways to flatten the loss curve.

[0263] For example, FIG. 61 is a diagram illustrating a side view of amirror for use with a VIPA to provide chromatic dispersion, and whichwill flatten the loss curve, according to an embodiment of the presentinvention. Referring now to FIG. 61, a mirror 704 could be a cone shapedmirror, a modified cone shaped mirror, a flat mirror, or any other shapemirror. FIG. 61 shows positions P, Q and R in the side view. PositionsP, Q and R corresponds, respectively to points 274, 270 and 272,respectively, in FIG. 14. Light at a shorter wavelength is focused atpoint 274 or P, and light at a longer wavelength is focused at point 272or R.

[0264] The reflectivity on mirror 740 is modulated along the angulardispersion direction of the VIPA. That is, the reflectivity at theposition Q is lowest, to thereby provide a higher loss, and thereflectivity at the position P and R is higher, to thereby provide alower loss. Therefore, the power of the reflected light is reduced nearthe center of the WDM channel, and thus the loss curve is flattened. Tomodify the reflectivity, a layer of light absorbing material may becoated near position Q or, in the case of a multi-layer mirror, thethickness of one or more layer may be modulated.

[0265] This modulation of the reflectivity can be effectively achievedby patterning the mirror instead of actually modulating thereflectivity, if the VIPA is used with a mirror which is not a cone ormodified cone shape, tat is, if the VIPA is used with a mirror such as,for example, mirror 254 in FIGS. 14, 20(A), 20(B), or the mirror shapesin FIGS. 28(A) through 28(F).

[0266] For example, FIG. 62 is a diagram illustrating a front view of amirror 750, according to an embodiment of the present invention.Referring now to FIG. 62, mirror 750 is patterned as illustrated in thefigure, to change the reflectivity of mirror 750. Here, the width ofmirror 750 is smaller than the focused beam size 760 near the positionQ, and therefore, the light power reflected from near position Q isreduced.

[0267] FIGS. 63(A), 63(B) and 63(C) are diagrams illustrating anotherway to modulate the effective reflectivity in the case of a VIPA usedwith a mirror 770 which is not a cone or modified cone shape, accordingto an embodiment of the present invention. More specifically, FIGS.63(A), 63(B) and 63(C) illustrate a top view of incident beam 780 onmirror 770 at positions P, Q and R, respectively. As illustrated inFIGS. 63(A), 63(B) and 63(C), instead of modulating the reflectivity,the mirror angle in the top view is changed. In previously describedembodiments of the present invention, such as that in FIG. 14, themirror is preferably perpendicular to the average light incident anglein the top view. However, if the mirror is tilted in the top view, as inFIGS. 63(A), 63(B) and 63(C), the reflected light is deflected and thecoupling efficiency to the output fiber is reduced. At positions P andR, incident light 780 is perpendicular to mirror 770 and the light isfully returned to the output fiber. On the other hand, at position Q,mirror 770 is tilted in the top view and the reflected light is slightlydiverged from the output fiber direction. This causes an excess loss andflattening Of the loss curve. By changing this tilting angle of mirror770 in the top view gradually along the angular dispersion direction ofthe VIPA, the excess loss to flatten the loss curve can be effectivelyproduced.

[0268] The changing of the mirror angle as in FIGS. 63(A), 63(B) and63(C), and the patterning of the mirror as in FIG. 62, could be used inthe above-described apparatuses which use a VIPA in combination with amirror which is not cone or modified cone shaped. This is because, inthe case of a cone or modified cone shaped mirror, the light at awavelength may be focused effectively at different positions on themirror in the top view, and therefore, the mirror should not bepatterned or tilted in the top view.

[0269] As described above, a mirror is used to reflect light back into aVIPA. Thus, a mirror can be referred to as a “light returning device”which returns light back to the VIPA. However, the present invention isnot limited to the use of a mirror as a light returning device. Forexample, a prism (instead of a mirror) can be used as a light returningdevice to return light back to the VIPA. Moreover, various combinationsof mirrors and/or prisms, or lens apparatuses can be used as a lightreturning device to return light back to VIPA.

[0270] In various embodiments of the present invention, a lens is usedto focus light from a VIPA to a mirror, and to direct the returninglight from the mirror back to the VIPA. See, for example, the operationof lens 252 in FIG. 13. However, the present invention is not limited tousing a lens for this purpose. Instead, other types of light directingdevices can be used in place of the lens. For example, a mirror can beused in place of lens 252 to focus the light from the VIPA, and todirect the returning light back to the VIPA.

[0271] In the above embodiments of the present invention, a VIPA hasreflecting films to reflect light. For example, FIG. 8 illustrates aVIPA 76 having reflecting films 122 and 124 to reflect light. However,it is not intended for a VIPA to be limited to the use of “film” toprovide a reflecting surface. Instead, the VIPA must simply haveappropriate reflecting surfaces, and these reflecting surfaces may ormay not be formed by “film”.

[0272] Further, in the above embodiments of the present invention, aVIPA includes a transparent glass plate in which multiple reflectionoccurs. For example, FIG. 8 illustrates a VIPA 76 having a transparentglass plate 120 with reflecting surfaces thereon. However, it is notintended for a VIPA to be limited to the use of a glass material, or anytype of “plate”, to separate the reflecting surfaces. Instead, thereflecting surfaces must simply be maintained to be separated from eachother by some type of spacer. For example, the reflecting surfaces of aVIPA can be separated by “air”, without having a glass platetherebetween. Therefore, the reflecting surfaces can be described asbeing separated by a transparent material which is, for example, opticalglass or air.

[0273] According to the above embodiments of the present invention, anapparatus uses a VIPA to compensate for chromatic dispersion. For thispurpose, the embodiments of the present invention are not intended to belimited to a specific VIPA configuration. Instead, any of the differentVIPA configurations discussed herein, or those disclosed in U.S.application Ser. No. 08/685,362, which is incorporated herein byreference, can be used in an apparatus to compensate for chromaticdispersion. For example, the VIPA may or may not have a radiationwindow, and the reflectances on the various surfaces of the VIPA are notintended to be limited to any specific examples.

[0274] The present invention relates to a VIPA dispersion compensator.The term “VIPA dispersion compensator” refers to an apparatus which usesa VIPA to produce chromatic dispersion, such as those described herein.For example, the apparatuses in FIGS. 13, 19, 32, 42, 44 and 48(A),among others, show a VIPA dispersion compensator.

[0275] Although a few preferred embodiments of the present inventionhave been shown and described, it would be appreciated by those skilledin the art that changes may be made in these embodiments withoutdeparting from the principles and spirit of the invention, the scope ofwhich is defined in the claims and their equivalents.

What is claimed is:
 1. An apparatus comprising: a virtually imagedphased array (VIPA) generator receiving an input light at a respectivewavelength and producing a corresponding collimated output lighttraveling from the VIPA generator in a direction determined by thewavelength of the input light; and a reflecting surface reflecting theoutput light back to the VIPA generator, the reflecting surface havingdifferent curvatures at different positions along a directionperpendicular to a plane which includes the traveling directions ofcollimated output light from the VIPA generator for input light atdifferent wavelengths.
 2. An apparatus as in claim 1, furthercomprising: a lens or mirror focusing the output light traveling fromthe VIPA generator onto the reflecting surface so that the reflectingsurface reflects the output light, the reflected light being directed bysaid lens or mirror back to the VIPA generator.
 3. An apparatus as inclaim 1, wherein the reflecting surface has a cone or modified coneshape.
 4. An apparatus as in claim 2, wherein the reflecting surface ismovable in or around a focal plane of the lens.
 5. An apparatus as inclaim 2, wherein the reflecting surface has a cone or modified coneshape.
 6. An apparatus as in claim 2, wherein the reflecting surfacetouches a focal plane of the lens along a line which is in the focalplane and is perpendicular to the light traveling directions of thecollimate output light from the VIPA.
 7. An apparatus as in claim 1,wherein the reflecting surface is movable in the direction of said line.8. An apparatus as in claim 2, further comprising: an angular dispersiveelement between the VIPA generator and said lens or mirror, the angulardispersive element having an angular dispersion direction which isperpendicular to said plane.
 9. An apparatus as in claim 8, wherein theangular dispersive element is a transmission type diffraction grating, areflection type diffraction grating or a holographic grating.
 10. Anapparatus as in claim 1, wherein the input light received by the VIPAgenerator has a double-hump shaped far field distribution.
 11. Anapparatus as in claim 1, further comprising: means for causing the inputlight received by the VIPA generator to have a double-hump shaped farfield distribution.
 12. An apparatus as in claim 1, further comprising:at least one phase mask causing the input light received by the VIPAgenerator to have a double-hump shaped far field distribution.
 13. Anapparatus as in claim 1, further comprising: a fiber providing the inputlight to the VIPA generator; and at least one phase mask on the fiber tocause the input light received by the VIPA generator to have adouble-hump shaped far field distribution.
 14. An apparatus as in claim1, further comprising: at least one phase mask on a surface of the VIPAgenerator to cause the input light received by the VIPA generator tohave a double-hump shaped far field distribution.
 15. An apparats as inclaim 1, wherein the input light is a wavelength division multiplexed(WDM) light having a plurality of channels, each channel having anamount of chromatic dispersion corresponding to wavelength and due totraveling through a transmission line, and parameters of the reflectingsurface cause the apparatus to provide chromatic dispersion to eachchannel in the same amount but opposite sign to that due to travelingthrough the transmission line.
 16. An apparatus as in claim 1, whereinthe input light has an associated loss curve, and the apparatus furthercomprises an excess loss component adding loss to the input light toflatten the loss curve.
 17. An apparatus comprising: a virtually imagedphased array (VIPA) generator receiving an input light at a respectivewavelength and producing a corresponding collimated output lighttraveling from the VIPA generator in a direction determined by thewavelength of the input light, the output light thereby being spatiallydistinguishable from an output light produced for an input light at adifferent wavelength; reflecting surface having a cone or modified coneshape; and a lens or mirror focusing the output light traveling from theVIPA generator onto the reflecting surface so that the reflectingsurface reflects the output light, the reflected light being directed bythe said lens or mirror back to the VIPA generator.
 18. An apparatus asin claim 17, wherein the cone or modified cone shape of the reflectingsurface corrects for non-uniform chromatic dispersion.
 19. An apparatusas in claim 17, wherein the cone or modified cone shaped reflectingsurface is movable in direction which is perpendicular to an angulardispersion direction of the VIPA generator.
 20. An apparatus as in clam17, wherein the reflecting surface is movable in a directionperpendicular to a plane which includes the traveling directions ofcollimated output light from the VIPA generator for input light atdifferent wavelengths.
 21. An apparatus as in claim 17, wherein thereflecting surface is movable in or near a focal plane of said lens ormirror.
 22. An apparatus as in claim 17, further comprising: an angulardispersive element between the VIPA generator and the lens.
 23. Anapparatus as in claim 22, wherein the angular dispersive element has anangular dispersion direction which is perpendicular to an angulardispersion direction of the VIPA generator.
 24. An apparatus as in claim22, wherein the angular dispersive element is a transmission typediffraction grating, a reflection type diffraction grating or aholographic grating.
 25. An apparatus as in claim 17, wherein the inputlight received by the VIPA generator has a double-hump shaped far fielddistribution.
 26. An apparatus as in claim 17, further comprising: meansfor causing the input light received by the VIPA generator to have adouble-hump shaped far field distribution.
 27. An apparatus as m claim17, further comprising: at least one phase mask causing the input lightreceived by the VIPA generator to have a double-hump shaped far fielddistribution.
 28. An apparatus as claim 17, further comprising: a fiberproviding the input light to the VIPA generator; and at least one phasemask on the fiber to cause the input light received by the VIPAgenerator to have a double-hump shaped far field distribution.
 29. Anapparatus as in claim 17, further comprising: at least one phase mask ona surface of the VIPA generator to cause the input light received by theVIPA generator to have a double-hump shaped far field distribution. 30.An apparatus as in claim 17, wherein the input light is a wavelengthdivision multiplexed (WDM) light having a plurality of channels, eachchannel having an amount of chromatic dispersion corresponding towavelength and due to traveling through a transmission line, andparameters of at least one of said reflecting surface and said lens ormirror cause the apparatus to provide chromatic dispersion to eachchannel in the same amount but opposite sign to that due to travelingthrough the transmission line.
 31. An apparatus as in claim 17, whereinthe input light has an associated loss curve, and the apparatus furthercomprises an excess loss component adding loss to the input light toflatten the loss curve.
 32. An apparatus comprising: an angulardispersive component having a passage area to receive light into, and tooutput light from, the angular dispersive component, the angulardispersive component receiving, through the passage area, an input lighthaving a respective wavelength within a continuous range of wavelengths,and causing multiple reflection of the input light to produceself-interference that forms a collimated output light which travelsfrom the angular dispersive component along a direction determined bythe wavelength of the input light and is thereby spatiallydistinguishable from an output light formed for an input light havingany other wavelength within the continuous range of wavelengths; and areflecting surface reflecting the output light back to the angulardispersive component to undergo multiple reflection in the angulardispersive component and then be output from the passage area, thereflecting surface having different curvatures at different positionsalong a direction which is perpendicular to a plane which includes thetravel direction of collimated output light from the angular dispersivecomponent for input light at different wavelengths.
 33. An apparatus asin claim 32, further comprising: a lens or mirror focusing the outputlight traveling from the angular dispersive component onto thereflecting surface so that the reflecting surface reflects the outputlight, the reflected light being directed by said lens or mirror back tothe angular dispersive component.
 34. An apparatus as in claim 32,wherein the reflecting surface has a cone or modified cone shape.
 35. Anapparatus as in claim 33, wherein the reflecting surface has a cone ormodified cone shape.
 36. An apparatus as in claim 32, wherein thereflecting surface is movable in a direction perpendicular to saidplane.
 37. An apparatus as in claim 35, wherein the reflecting surfaceis movable in a direction perpendicular to said plane.
 38. An apparatusas in claim 33, wherein the angular dispersive component is a firstangular dispersive component, the apparatus further comprising: a secondangular dispersive component between the first angular dispersivecomponent and said lens or mirror, the first angular dispersivecomponent having an angular dispersion direction which is perpendicularto said plane.
 39. An apparatus as in claim 38, wherein the secondangular dispersive component is a transmission type diffraction grating,a reflection type diffraction grating or a holographic grating.
 40. Anapparatus as in claim 32, wherein the input light received by theangular dispersive component has a double-hump shaped far fielddistribution.
 41. An apparatus as in claim 32, further comprising: meansfor causing the input light received by the angular dispersive componentto have a double-hump shaped far field distribution.
 42. An apparatus asin claim 32, further comprising: at least one phase mask causing theinput light received by the angular dispersive component to have adouble-hump shaped far field distribution.
 43. An apparatus as in claim32, further comprising: a fiber providing the input light to the angulardispersive component; and at least one phase mask on the fiber to causethe input light received by the angular dispersive component to have adouble-hump shaped far field distribution.
 44. An apparatus as in claim32, further comprising: at least one phase mask on a surface of theangular dispersive component to cause the input light received by theangular dispersive component to have a double-hump shaped far fielddistribution.
 45. An apparatus comprising: an angular dispersivecomponent having a passage area to receive light into, and to outputlight from, the angular dispersive component, the angular dispersivecomponent receiving, through the passage area, a line focused inputlight and causing multiple reflection of the input light to produceself-interference that forms a collimated output light which travelsfrom the angular dispersive component along a direction determined bythe wavelength of the input light and is thereby spatiallydistinguishable from an output light formed for an input light having adifferent wavelength; and a reflecting surface reflecting the outputlight back to the angular dispersive component to undergo multiplereflection in the angular dispersive component and then be output fromthe passage area, the reflecting surface having different curvatures atdifferent positions along a direction which is perpendicular to a planewhich includes the travel direction of collimate output light from theangular dispersive component for input light at different wavelengths.46. An apparatus as in claim 45, further comprising: a lens or mirrorfocusing the output Light traveling from the angular dispersivecomponent onto the reflecting surface so that the reflecting surfacereflects the output light, the reflected light being directed by saidlens or mirror back to the angular dispersive component.
 47. Anapparatus as in claim 45, wherein the reflecting surface has a cone ormodified cone shape.
 48. An apparatus as in claim 46, wherein thereflecting surface has a cone or modified cone shape.
 49. An apparatusas in claim 45, wherein the-reflecting surface is movable in a directionperpendicular to said plane.
 50. An apparatus as in claim 46, whereinthe reflecting surface is movable in a direction perpendicular to saidplane.
 51. An apparatus as in claim 46, wherein the angular dispersivecomponent is a first angular dispersive component, the apparatus furthercomprising: a second angular dispersive component between the firstangular dispersive component and said lens or mirror, the second angulardispersive component having an angular dispersion direction which isperpendicular to said plane.
 52. An apparatus as in claim 51, whereinthe second angular dispersive component is a transmission typediffraction grating, a reflection type diffraction grating or aholographic grating.
 53. An apparatus as in claim 45, wherein the inputlight received by the angular dispersive component has a double-humpshaped far field distribution.
 54. An apparatus as in claim 45, furthercomprising: means for causing the input light received by the angulardispersive component to have a double-hump shaped far fielddistribution.
 55. An apparatus as in claim 45, further comprising: atleast one phase mask causing the input light received by the angulardispersive component to have a double-hump shaped far fielddistribution.
 56. An apparatus as in claim 45, further comprising: afiber providing the input light to the angular dispersive component; andat least one phase mask on the fiber to cause the input light receivedby the angular dispersive component to have a double-hump shaped farfield distribution.
 57. An apparatus as in claim 45, further comprising:at least one phase mask on a surface of the angular dispersive componentto cause the input light received by the angular dispersive component tohave a double-hump shaped far field distribution.
 58. An apparatuscomprising: first and second reflecting surfaces, the second reflectingsurface having a reflectivity which causes a portion of light incidentthereon to be a therethrough, where an input light at a respectivewavelength is focused into a line, and the first and second reflectingsurfaces are positioned so that the input light radiates from the lineto be reflected a plurality of times between the first and secondreflecting surfaces and thereby cause a plurality of lights to betransmitted through the second reflecting surface, the plurality oftransmitted lights interfering with each other to produce a collimatedoutput light which travels from the second reflecting surface along adirection determined by the wavelength of the input light, and isthereby specially distinguishable from an output light formed for aninput light having a different wavelength; and a mirror surfacereflecting output the light back to the second reflecting surface topass through the second reflecting surface and undergo multiplereflection between the first and second reflecting surfaces, the mirrorsurface having different curvatures at different positions along adirection which is perpendicular to a plane which includes the traveldirection of collimated output light from the second reflecting surfacefor input light at different wavelengths.
 59. An apparatus as in claim58, further comprising: a lens or mirror focusing the output lighttraveling from the second reflecting surface onto the mirror surface sothat the mirror surface reflects the output light, the reflected lightbeing directed by the said lens or mirror back to the second reflectingsurface.
 60. An apparatus as in claim 58, wherein the mirror surface hasa cone or modified cone shape.
 61. An apparatus as in claim 59, whereinthe mirror surface has a cone or modified cone shape.
 62. An apparatusas in claim 59, wherein the mirror surface is movable in a directionwhich is perpendicular to said plane.
 63. An apparatus as in claim 59,further comprising: an angular dispersive component between the secondreflecting surface and said lens or mirror, the angular dispersivecomponent having an angular dispersion direction which is perpendicularto said plane.
 64. An apparatus as in claim 63, wherein the angulardispersive component is a transmission type diffraction grating, areflection type diffraction grating or a holographic grating.
 65. Anapparatus as in claim 58, wherein the input light has a double-humpshaped far field distribution.
 66. An apparatus as in claim 58, furthercomprising: means for causing the input light to have a double-humpshaped far field distribution.
 67. An apparatus as in claim 58, furthercomprising: at least one phase mask causing the input light to have adouble-hump shaped far field distribution.
 68. An apparatus as in claim58, further comprising: a fiber providing the input light to be focusedinto the line; and at least one phase mask on the fiber to cause theinput light to have a double-hump shaped far field distribution.
 69. Anapparatus as in claim 58, further comprising: at least one phase mask onone of the group consisting of first and second reflecting surfaces, tocause the input light to have a double-hump shaped far fielddistribution.
 70. An apparatus comprising: first and second reflectingsurfaces, the second reflecting surface having a reflectivity whichcauses a portion of light incident thereon to be transmittedtherethrough; means for causing an input light at a respectivewavelength and focused into a line to radiate from the line to bereflected a plurality of times between the first and second reflectingsurfaces and thereby cause a plurality of lights to be transmittedthrough the second reflecting surface, the plurality of transmittedlights interfering with each other to produce a collimated output lighttraveling from the second reflecting surface in a direction determinedby the wavelength of the input light, and is thereby spatiallydistinguishable from an output light produced for an input light at adifferent wavelength; a mirror surface having a cone or modified coneshape; and a lens or mirror focusing the output light traveling from thesecond reflecting surface onto the mirror surface so that the mirrorsurface reflects the output light, the reflected light being directed bysaid lens or mirror back to the second reflecting surface.
 71. Anapparatus comprising: a virtually imaged phased array (VIPA) generatorreceiving a line focused wavelength division multiplexed light includinglight at first and second wavelengths, and producing collimated firstand second output lights corresponding, respectively, to the first andsecond wavelengths, the first and second output lights traveling fromthe VIPA generator in first and second directions, respectively,determined by the first and second wavelengths, respectively; a lens orlight directing mirror focusing the first and second output lightstraveling from the VIPA generator; first and second mirrors each havinga cone shape or a modified cone shape for producing a uniform chromaticdispersion; and a wavelength filter filtering light focused by said lensor light directing mirror so that light at the first wavelength isfocused to the first mirror and reflected by the first mirror, and lightat the second wavelength is focused to the second mirror and reflectedby the second mirror, the reflected first and second lights beingdirected by the wavelength filter and said lens or light directingmirror back to the VIPA generator.
 72. An apparatus as in claim 71,wherein the first and second mirrors are movable to change the amount ofchromatic dispersion provided to light at the first and secondwavelengths, respectively.
 73. An apparatus comprising: first and secondreflecting surfaces, the second reflecting surface having a reflectivitywhich causes a portion of light incident thereon to be transmittedtherethrough, where a wavelength division multiplexed (WDM) lightincluding light at first and second wavelengths is focused into a line,and the first and second reflecting sure are positioned so that the WDMlight radiates from the line to be reflected a plurality of timesbetween the first and second reflecting surfaces and thereby cause aplurality of lights to be transmitted through the second reflectingsurface, the plurality of transmitted lights interfering with each otherto produce collimate first and second output lights corresponding,respectively, to the first and second wavelengths, the first and secondoutput lights traveling from the second reflecting surface in first andsecond directions, respectively, determined by the first and secondwavelengths, respectively; a lens or light directing mirror focusing thefirst and second output lights traveling from the second reflectingsurface; first and second mirrors each having a cone shape or a modifiedcone shape for producing a uniform chromatic dispersion; and awavelength filter filtering light focused by said lens or lightdirecting mirror so that light at the first wavelength is focused to thefirst mirror and reflected by the first mirror, and light at the secondwavelength is focused to the second mirror and reflected by the secondmirror, the reflected first and second lights being directed by thewavelength filter and said lens or light directing mirror back to thesecond reflecting surface to pass through the second reflecting surfaceand undergo multiple reflection between the first and second surfaces.74. An apparatus as in claim 73, wherein the first and second mirrorsare movable to change the amount of chromatic dispersion provided tolight at the first and second wavelengths, respectively.
 75. Acommunication system comprising: an optical transmission line; atransmitter transmitting an optical signal through the transmissionline; a receiver receiving optical signal from the transmission line;and a compensation device operatively connected in one of the groupconsisting of the transmitter, the receiver and the transmission line,to provide dispersion slope or higher order dispersion to the opticalsignal, the compensation device comprising a virtually imaged phasedarray (VIPA) generator receiving the optical signal as a line focusedinput light and producing a corresponding collimated output lighttraveling from the VIPA generator in a direction determined by awavelength of the input light, a mirror having a cone or modified coneshape, and a light directing device focusing the output light travelingfrom the VIPA generator onto the mirror so that the mirror reflects theoutput light, the reflected light being directed by the light directingdevice back to the VIPA generator.
 76. A communication systemcomprising: an optical transmission line; a transmitter transmitting anoptical signal through the transmission line; a receiver receivingoptical signal from the transmission line; and a compensation deviceoperatively connected in one of the group consisting of the transmitter,the receiver and the transmission line, to provide dispersion slope orhigher order dispersion to the optical signal, the compensation devicecomprising first and second reflecting surface, the second reflectingsurface having a reflectivity which causes a portion of light incidentthereon to be transmitted therethrough, where the optical signal isfocused into a line as a line focused input light to the compensationdevice, and the first and second reflecting surfaces are positioned sothat the input light radiates from the line to be reflected a pluralityof times between the first and second reflecting surfaces and therebycause a plurality of lights to be transmitted through the secondreflecting surface, the plurality of transmitted lights interfering witheach other to produce a collimated output light which travels from thesecond reflecting surface along a direction determined by a wavelengthof the input light, and is thereby specially distinguishable from anoutput light formed for an input light having a different wavelength,and a mirror reflecting output the light back to the second reflectingsurface to pass through the second reflecting surface and undergomultiple reflection between the first and second reflecting surfaces,the mirror having different curvatures at different positions along adirection which is perpendicular to a plane which includes the traveldirection of collimated output light from the second reflecting surfacefor input light at different wavelengths.
 77. An apparatus comprising: avirtually imaged phased array (VIPA) generator receiving an input lightat a respective wavelength and having a double-hump shaped far fielddistribution, and producing a corresponding collimated output lighttraveling from the VIPA generator in a direction determined by thewavelength of the input light; and a reflecting surface reflecting theoutput light back to the VIPA generator.
 78. An apparatus as in claim77, further comprising: a lens or mirror focusing the output lighttraveling from the VIPA generator onto the reflecting surface so thatthe reflecting surface reflects the output light, the reflected lightbeing directed by said lens or mirror back to the VIPA generator.
 79. Anapparatus as in claim 77, further comprising: means for causing theinput light received by the VIPA generator to have a double-hump shapedfar field distribution.
 80. An apparatus as in claim 77, furthercomprising: at least one phase mask causing the input light received bythe VIPA generator to have a double-hump shaped far field distribution.81. An apparatus as in claim 77, further comprising: a fiber providingthe input light to the VIPA generator; and at least one phase mask onthe fiber to cause the input light received by the VIPA generator tohave a double-hump shaped far field distribution.
 82. An apparatus as inclaim 77, further comprising: at least one phase mask on a surface ofthe VIPA generator to cause the input light received by the VIPAgenerator to have a double-hump shaped far field distribution.
 83. Anapparatus comprising: a virtually imaged phased array (VIPA) generatorreceiving an input light at a respective wavelength and having adouble-hump shaped far field distribution, and producing a correspondingcollimated output light traveling from the VIPA generator in a directiondetermined by the wavelength of the input light, the output lightthereby being spatially distinguishable from an output light producedfor an input light at a different wavelength; a reflecting surface; anda lens or mirror focusing the output light traveling from the VIPAgenerator onto the reflecting surface so that the reflecting surfacereflects the output light, the reflected light being directed by saidlens or mirror back to the VIPA generator.
 84. An apparatus as in claim83, further comprising: means for causing the input light received bythe VIPA generator to have a double-hump shaped far field distribution.85. An apparatus as in claim 83, further comprising: at least one phasemask causing the input light received by the VIPA generator to have adouble-hump shaped far field distribution.
 86. An apparatus as in claim83, further comprising: a fiber providing the input light to the VIPAgenerator; and at least one phase mask on the fiber to cause the inputlight received by the VIPA generator to have a double-hump shaped farfield distribution.
 87. An apparatus as in clam 83, further comprising:at least one phase mask on a surface of the VIPA generator to cause theinput light received by the VIPA generator to have a double-hump shapedfar field distribution.
 88. An apparatus comprising: an angulardispersive component having a passage area to receive light into, and tooutput light from, the angular dispersive component, the angulardispersive component receiving, through the passage area, an input lighthaving a respective wavelength within a continuous range of wavelengthsand having a double-hump shaped far field distribution, and causingmultiple reflection of the input light to produce self-interference thatforms a collimated output light which travels from the angulardispersive component along a direction determined by the wavelength ofthe input light and is thereby spatially distinguishable from an outputlight formed for an input light having any other wavelength within thecontinuous range of wavelengths; and a reflecting surface reflecting theoutput light back to the angular dispersive component to undergomultiple reflection in the angular dispersive component and then beoutput from the passage area.
 89. An apparatus as in claim 88, furthercomprising: a lens or mirror focusing the output light traveling fromthe angular dispersive component onto the reflecting surface so that thereflecting surface reflects the output light, the reflected light beingdirected by said lens or mirror back to the angular dispersivecomponent.
 90. An apparatus as in claim 88, further comprising: meansfor causing the input light received by the angular dispersive componentto have a double-hump shaped far field distribution.
 91. An apparatus asin claim 88, further comprising: at least one phase mask causing theinput light received by the angular dispersive component to have adouble-hump shaped far field distribution.
 92. An apparatus as in claim88, further comprising: a fiber providing the input light to the angulardispersive component; and at least one phase mask on the fiber to causethe input light received by the angular dispersive component to have adouble-bump shaped far field distribution.
 93. An apparatus as in claim88, further comprising: at least one phase mask on a surface of theangular dispersive component to cause the input light received by theangular dispersive component to have a double-hump shaped far fielddistribution.
 94. An apparatus comprising: an angular dispersivecomponent having a passage area to receive light into, and to outputlight from, the angular dispersive component, the angular dispersivecomponent receiving, through the passage area, a line focused inputlight having a double-hump shaped far field distribution and causingmultiple reflection of the input light to produce self-interference thatforms a collimated output light which travels from the angulardispersive component along a direction determined by the wavelength ofthe input light and is thereby spatially distinguishable from an outputlight formed for an input light having a different wavelength; and areflecting surface reflecting the output light back to the angulardispersive component to undergo multiple reflection in the angulardispersive component and then be output from the passage area.
 95. Anapparatus as in claim 94, further comprising: a lens or mirror focusingthe output light traveling from the angular dispersive component ontothe reflecting surface so that the reflecting surface reflects theoutput light, the reflected light being directed by the lens or mirrorback to the angular dispersive component.
 96. An apparatus as in claim94, further comprising: means for causing the input light received bythe angular dispersive component to have a double-hump shaped far fielddistribution.
 97. An apparatus as in claim 94, further comprising: atleast one phase mask causing the input light received by the angulardispersive component to have a double-hump shaped far fielddistribution.
 98. An apparatus as in claim 94, further comprising: afiber providing the input light to the angular dispersive component; andat least one phase mask on the fiber to cause the input light receivedby the angular dispersive component to have a double-hump shaped farfield distribution.
 99. An apparatus as in claim 94, further comprising:at least one phase mask on a surface of the angular dispersive componentto cause the input light received by the angular dispersive component tohave a double-hump shaped far field distribution.
 100. An apparatuscomprising: first and second reflecting surfaces, the second reflectingsurface having a reflectivity which causes a portion of light incidentthereon to be transmitted therethrough, where an input light at arespective wavelength is focused into a line and has a double-humpshaped far field distribution, and the first and second reflectingsurfaces are positioned so that the input light radiates from the lineto be reflected a plurality of times between the first and secondreflecting surfaces and thereby cause a plurality of lights to betransmitted through the second reflecting surface, the plurality oftransmitted lights interfering with each other to produce a collimatedoutput light which travels from the second reflecting surface along adirection determined by the wavelength of the input light, and isthereby specially distinguishable from an output light formed for aninput light having a different wavelength; and a mirror surfacereflecting output the light back to the second reflecting surface topass through the second reflecting surface and undergo multiplereflection between the first and second reflecting surfaces.
 101. Anapparatus as in claim 100, further comprising: a lens or light directingmirror focusing the output light traveling from the second reflectingsurface onto the mirror surface so that the mirror surface reflects theoutput light, the reflected light being directed by said lens or lightdirecting mirror back to the second reflecting surface.
 102. Anapparatus as in claim 100, further comprising: means for causing theinput light to have a double-hump shaped far field distribution.
 103. Anapparatus as in claim 100, further comprising: at least one phase maskcausing the input light to have a double-hump shaped farfield-distribution.
 104. An apparatus as in claim 100, furthercomprising: a fiber providing the input light to be focused into theline; and at least one phase mask on the fiber to cause the input lightto have a double-hump shaped far field distribution.
 105. An apparatusas in claim 100, further comprising: at least one phase mask on one ofthe group consisting of first and second reflecting surfaces, to causethe input light to have a double-hump shaped far field distribution.106. An apparatus comprising: a virtually imaged phased array (VIPA)generator receiving a line focused input light at a respectivewavelength and producing a corresponding collimated output lighttraveling from the VIPA generator in a direction determined by thewavelength of the input light, the output light thereby being spatiallydistinguishable from an output light produced for an input light at adifferent wavelength, the input light having an associated loss curve;and an excess loss component adding loss to the input light to flattenthe loss curve.
 107. An apparatus as in claim 106, wherein the excessloss component is one of the group consisting of a Mach-Zehnderinterferometer, a Fabry-Perot interferometer, an optical interferometerand a wavelength filter.
 108. An apparatus comprising: a virtuallyimaged phased array (VIPA) generator receiving a line focused inputlight at a respective wavelength and producing a correspondingcollimated output light traveling from the VIPA generator in a directiondetermined by the wavelength of the input light, the VIPA generatorhaving a corresponding angular dispersion direction; and a reflectingsurface reflecting the output light back to the VIPA generator toprovide chromatic dispersion or higher order dispersion to the inputlight, wherein reflectivity of the reflecting surface is modulated alongthe angular dispersion direction of the VIPA generator.
 109. Anapparatus as in claim 108, wherein the reflecting surface is one of thegroup consisting of a cone shaped mirror, a modified cone shaped mirrorand a cylindrical mirror.
 110. An apparatus comprising: a virtuallyimaged phased array (VIPA) generator receiving a line focused inputlight at a respective wavelength and producing a correspondingcollimated output light traveling from the VIPA generator in a directiondetermined by the wavelength of the input light, the VIPA generatorhaving a corresponding angular dispersion direction and the input lighthaving an associated loss curve; a reflecting surface; and a lens ormirror focusing the output light traveling from the VIPA generator ontothe reflecting surface so that the reflecting surface reflects theoutput light, the reflected light being directed by the said lens ormirror back to the VIPA generator, wherein the reflecting surface ispatterned to flatten loss curve.